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Spiral similarity
Page made by vladimir.shelomovskii@gmail.com, vvsss
Contents
[hide]
1 Definition
2 Simple problems
2.1 Explicit spiral similarity
2.2 Hidden spiral symilarity
2.3 Linearity of the spiral symilarity
2.4 Construction of a similar triangle
2.5 Center of the spiral symilarity for similar triangles
2.6 Spiral similarity in rectangle
2.7 Common point for 6 circles
2.8 Three spiral similarities
2.9 Superposition of two spiral similarities
2.10 Spiral similarity for circles
2.11 Remarkable point for spiral similarity
2.12 Remarkable point for pair of similar triangles
2.13 Remarkable point’s problems
2.13.1 Problem 1
2.13.2 Problem 2
2.13.3 Problem 3
2.13.4 Problem 4
2.13.5 Solutions
2.14 Japan Mathematical Olympiad Finals 2018 Q2
Definition
A spiral similarity is a plane transformation composed of a rotation of the plane and a dilation of the plane having the common center. The order in which the composition is taken is not important.
Any two directly similar figures are related either by a translation or by a spiral similarity (directly similar figures are similar and have the same orientation).
The transformation is linear and transforms any given object into an object homothetic to given.
On the complex plane, any spiral similarity can be expressed in the form where is a complex number. The magnitude is the dilation factor of the spiral similarity, and the argument is the angle of rotation.
The spiral similarity is uniquely defined by the images of two distinct points. It is easy to show using the complex plane.
Let with corresponding complex numbers and so For any points and the center of the spiral similarity taking to point is also the center of a spiral similarity taking to This fact explain existance of Miquel point.
Case 1 Any line segment can be mapped into any other using the spiral similarity. Notation is shown on the diagram.
is circle is circle
is any point of is circle is the image under spiral symilarity centered at
is the dilation factor,
is the angle of rotation.
Case 2 Any line segment can be mapped into any other using the spiral similarity. Notation is shown on the diagram. is circle (so circle is tangent to is circle tangent to is any point of is circle is the image under spiral symilarity centered at is the dilation factor,
is the angle of rotation.
Simple problems
Explicit spiral similarity
Given two similar right triangles and Find and
Solution
The spiral similarity centered at with coefficient and the angle of rotation maps point to point and point to point
Therefore this similarity maps to
Hidden spiral symilarity
Let be an isosceles right triangle Let be a point on a circle with diameter The line is symmetrical to with respect to and intersects at Prove that
Proof
Denote Let cross perpendicular to in point at point
Then
Points and are simmetric with respect so
The spiral symilarity centered at with coefficient and the angle of rotation maps to and to point such that
Therefore
Linearity of the spiral symilarity
Points are outside
Prove that the centroids of triangles and are coinsite.
Proof
Let where be the spiral similarity with the rotation angle and
A vector has two parameters, modulo and direction. It is not tied to a center of the spiral similarity. Therefore We use the property of linearity and get Let be the centroid of so
is the centroid of the
Construction of a similar triangle
Let triangle and point on sideline be given. Construct where lies on sideline and lies on sideline
Solution
Let be the spiral symilarity centered at with the dilation factor and rotation angle
so image of any point lies on The spiral symilarity centered at with the dilation factor and rotation angle maps into and therefore the found triangle is the desired one.
Center of the spiral symilarity for similar triangles
Let triangle and point on sideline be given. where lies on sideline and lies on sideline The spiral symilarity maps into Prove
a)
b) Center of is the First Brocard point of triangles and
Proof
a) Let be the spiral symilarity centered at with the dilation factor and rotation angle
Denote Similarly
b) It is well known that the three circumcircles and have the common point (it is in the diagram).
Therefore is cyclic and
Similarly,
Similarly,
Therefore, is the First Brocard point of
is cyclic Similarly,
Therefore is the First Brocard point of and
Therefore the spiral symilarity maps into has the center the angle of the rotation
Spiral similarity in rectangle
Let rectangle be given. Let point
Let points and be the midpoints of segments and respectively.
Prove that
Proof
Let be the midpoint
is a parallelogram
and are corresponding medians of and
There is a spiral similarity centered at with rotation angle that maps to Therefore
Common point for 6 circles
Let and point on sideline be given. where lies on sideline and lies on sideline
Denote
Prove that circumcircles of triangles have the common point.
Proof
so there is the spiral symilarity taking to Denote the center of the center of is the secont crosspoint of circumcircles of and but this center is point so these circles contain point . Similarly for another circles.
Three spiral similarities
Let triangle be given. The triangle is constructed using a spiral similarity of with center , angle of rotation and coefficient
A point is centrally symmetrical to a point with respect to
Prove that the spiral similarity with center , angle of rotation and coefficient taking to
Proof
Corollary
Three spiral similarities centered on the images of the vertices of the given triangle and with rotation angles equal to the angles of take to centrally symmetric to with respect to
Superposition of two spiral similarities
Let be the spiral similarity centered at with angle and coefficient
Let be spiral similarity centered at with angle and coefficient
Let
Prove: a) is the crosspoint of bisectors and
b)
Algebraic proof
We use the complex plane Let Then Geometric proof
Denote
Then
Let be the midpoint be the point on bisector such that be the point on bisector such that Then
is the crosspoint of bisectors and
Corollary
There is another pair of the spiral similarities centered at and with angle coefficients and
In this case
Spiral similarity for circles
Let circle cross circle at points and Point lies on
Spiral similarity centered at maps into
Prove that points and are collinear.
Proof
Arcs
Corollary
Let points and be collinear.
Then exist the spiral similarity centered at such that
Let circle cross circle at points and
Points and lie on
Let be the tangent to be the tangent to
Prove that angle between tangents is equal angle between lines and
Proof
There is the spiral similarity centered at such that Therefore angles between these lines are the same.
Remarkable point for spiral similarity
Circles and centered at points and respectively intersect at points and Points and are collinear. Point is symmetrical to with respect to the midpoint point Prove:
a) b)
Proof
a) cross in midpoint
b) is parallelogram
Denote
Corollary
Let points and be collinear. Then
Therefore is the crosspoint of the bisectors and
Remarkable point for pair of similar triangles
Let
Let the points and be the circumcenters of and
Let point be the midpoint of
The point is symmetric to with respect point
Prove:
a) point be the crosspoint of the bisectors and
b)
Proof
is parallelogram Denote
Similarly,
The statement that was proved in the previous section.
Remarkable point’s problems
Problem 1
Let a convex quadrilateral be given,
Let and be the midpoints of and respectively.
Circumcircles and intersect a second time at point
Prove that points and are concyclic.
Problem 2
Let triangle be given.
Let point lies on sideline
Denote the circumcircle of the as , the circumcircle of the as .
Let be the circumcenter of
Let circle cross sideline at point
Let the circumcircle of the cross at point
Prove that
Problem 3
The circles and are crossed at points and points
Let be the tangent to be the tangent to
Point is symmetric with respect to
Prove that points and are concyclic.
Problem 4
The circles and are crossed at points and points
Let be the tangent to be the tangent to
Points and lye on bisector of the angle
Points and lye on external bisector of the angle
Prove that and bisector are tangent to the circle
bisector is tangent to the circle
Solutions
Solutions are clear from diagrams.
In each case we use remarcable point as the point of bisectors crossing.
Solution 1
We use bisectors and . The points and are concyclic.
Solution 2 We use bisectors of and
Solution 3
We use bisectors of and .
is the circumcenter of
Circle is symmetric with respect diameter
Point is symmetric to with respect diameter
Therefore
Solution 4
Let
Let be midpoint be midpoint .
We need prove that and
Denote
The angle between a chord and a tangent is half the arc belonging to the chord.
is tangent to
is diameter Similarly, is diameter is tangent to
Let be the spiral similarity centered at
Points and are collinear Points and are collinear
Therefore is tangent to
Similarly, is tangent to
Japan Mathematical Olympiad Finals 2018 Q2
Given a scalene let and be points on lines and respectively, so that
Let be the circumcircle of and the reflection of across
Lines and meet again at and respectively.
Prove that and intersect on
Proof
Let be the orthocenter of
Point is symmetrical to point with respect to height
Point is symmetrical to point with respect to height
is centered at
is symmetrical with respect to heightline
is symmetrical to point with respect to height
is symmetrical to point with respect to height
The isosceles triangles
a) are concyclic.
b) is the spiral center that maps to maps to
Therefore are concyclic and are concyclic.
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11302 | https://www.marmetal.com/wp-content/uploads/2017/12/C260-Insert.pdf | C26000 Cartridge Brass, also known as 70 30, is copper alloyed with zinc. C260 Cartridge Brass is a yellow brass, most commonly found in tube, sheet and plate form. C260 is commonly called Cartridge Brass because it has traditionally been for ammunition cartridges and shells. 70 30 brass has a wide range of uses, including applications in architectural, electrical, consumer, construction and plumbing industries. Some common products produced from C26000 Cartridge Brass include bathroom fixtures, watch parts, terminal connectors, decorative hardware, radiator cores and pump cylinders. Density @ 68o F 0.308 lb/in3 Melting Range 1680-1750o F Hot Formability Fair Cold Formability Excellent Machinability rating (C360 = 100) 30 Brazing Excellent Soldering Excellent Gas-shielded arc welding Good Oxy-acetylene welding Good Carbon-arc welding Not recommended Coated metal-arc welding Not recommended Resistant welding: spot and seam Fair Resistance Welding: butt Good Temper Designation Tensile, min ksi (MPa) Tensile, max ksi (MPa) M20 As Hot-Rolled 41 (275) 51 (345) H01 Quarter-Hard 49 (340) 59 (405) H02 Half-Hard 57 (380) 67 (450) H03 Three-Quarter Hard 64 (425) 74 (595) H04 Hard 71 (470) 81 (540) H06 Extra Hard 83 (545) 92 (615) 2950 Turnpike Drive Hatboro, PA 19040 ph: 215-675-4645 fax: 215-675-9947 www.marmetal.com sales@marmetal.com UNS No. Copper Lead Iron Zinc C26000 68.5-71.5 0.07 max 0.05 max remainder C260 CARTRIDGE BRASS ASTM B19 ASTM B36 ASTM B135 |
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Fundamentals of Carrier Transport
Lundstrom, Mark
Abstract
Fundamentals of Carrier Transport explores the behavior of charged carriers in semiconductors and semiconductor devices for readers without an extensive background in quantum mechanics and solid-state physics. This second edition contains many new and updated sections, including a completely new chapter on transport in ultrasmall devices and coverage of "full band" transport. Lundstrom also covers both low- and high-field transport, scattering, transport in devices, and transport in mesoscopic systems. He explains in detail the use of Monte Carlo simulation methods and provides many homework exercises along with a variety of worked examples. What makes this book unique is its broad theoretical treatment of transport for advanced students and researchers engaged in experimental semiconductor device research and development.
Publication:
Fundamentals of Carrier Transport
Pub Date:November 2000 Bibcode:2000fct..book.....L
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Choose a calculation for weight W, mass m or gravity g. Enter two known values and the calculator solves for the third in your selected measurement units.
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In physics weight is a measure of the force of gravity acting upon an object. It is typically measured in newtons which signifies force. Mass describes how much an object resists a change in velocity in kg, and gravity is the acceleration force acting upon that object in m/s2.
The Weight Equation
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Variables in the Weight Equation
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g = gravity (acceleration due to the pull of gravity)
The Weight Calculator uses the formula W = mg, or weight W is equal to mass m times gravity g. Note that the standard units for weight calculations are N, kg and m/s2. If you enter other units of measure for your calculation the calculator will do the units conversion for you.
Weight is a force and gravity can be thought of as an acceleration due to the pull of gravity. The equation W = mg is a special case of Newton's second law of motion, F = ma, where force F equals mass m times acceleration a.
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Calculate gravity given weight and mass:
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If you were on a different planet the force of gravity would be different than it is on Earth. This reference table provides the gravitational force for the sun, moon and each planet in our solar system.
Planetary Gravity Table
Gravity
m/s2
Sun
274
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Venus
8.87
Earth
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Moon
1.62
Mars
3.71
Jupiter
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10.44
Uranus
8.87
Neptune
11.15
Pluto
0.58
Table source:
Planetary Fact Sheet - NASA
Standard gravity (gn): 1.00gn is equal to 9.80665 m/s2 gravity on Earth.
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11306 | https://chem.libretexts.org/Bookshelves/Physical_and_Theoretical_Chemistry_Textbook_Maps/Supplemental_Modules_(Physical_and_Theoretical_Chemistry)/Kinetics/06%3A_Modeling_Reaction_Kinetics/6.04%3A_Transition_State_Theory/6.4.01%3A_Eyring_equation | Skip to main content
6.4.1: Eyring equation
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6.4: Transition State Theory
7: Case Studies- Kinetics
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The Eyring Equation, developed by Henry Eyring in 1935, is based on transition state theory and is used to describe the relationship between reaction rate and temperature. It is similar to the Arrhenius Equation, which also describes the temperature dependence of reaction rates. However, whereas Arrhenius Equation can be applied only to gas-phase kinetics, the Eyring Equation is useful in the study of gas, condensed, and mixed-phase reactions that have no relevance to the collision model.
Introduction
The Eyring Equation gives a more accurate calculation of rate constants and provides insight into how a reaction progresses at the molecular level. The Equation is given below:
k=kBThe−(△H‡RT)e(△S‡R)(6.4.1.1)
Consider a bimolecular reaction:
A +B → C(6.4.1.2)
K=[C][A]B
where K is the equilibrium constant. In the transition state model, the activated complex AB is formed:
A + B ⇌ AB‡ → C(6.4.1.4)
K‡=[AB]‡[A]B
There is an energy barrier, called activation energy, in the reaction pathway. A certain amount of energy is required for the reaction to occur. The transition state, AB‡, is formed at maximum energy. This high-energy complex represents an unstable intermediate. Once the energy barrier is overcome, the reaction is able to proceed and product formation occurs.
The rate of a reaction is equal to the number of activated complexes decomposing to form products. Hence, it is the concentration of the high-energy complex multiplied by the frequency of it surmounting the barrier.
rate == v[AB‡] v[A][B]K‡(6.4.1.6)(6.4.1.7)
The rate can be rewritten:
rate = k[A]B
Combining Equations 6.4.1.8 and 6.4.1.7 gives:
k[A][B] k == v[A][B]K‡ vK‡(6.4.1.9)(6.4.1.10)
where
v is the frequency of vibration,
k is the rate constant and
K‡ is the thermodynamic equilibrium constant.
The frequency of vibration is given by:
v = kBTh(6.4.1.11)
where
kB is the Boltzmann's constant (1.381 x 10-23 J/K),
T is the absolute temperature in Kelvin (K) and
h is Planck's constant (6.626 x 10-34 Js).
Substituting Equation 6.4.1.11 into Equation 6.4.1.10 :
k = kBThK‡(6.4.1.12)
Equation ref is often tagged with another term (M1−m) that makes the units equal with M is the molarity and m is the molecularly of the reaction.
k = kBThK‡(M1−m)(6.4.1.13)
The following thermodynamic equations further describe the equilibrium constant:
ΔG‡ ΔG‡ == −RTlnK‡ ΔH‡ − TΔS‡(6.4.1.14)(6.4.1.15)
where ΔG‡ is the Gibbs energy of activation, ΔH‡ is the enthalpy of activation and ΔS‡ is the entropy of activation. Combining Equations 6.4.1.10 and 6.4.1.11 to solve for lnK‡ gives:
lnK‡ = −ΔH‡RT + ΔS‡R(6.4.1.16)
The Eyring Equation is finally given by substituting Equation 6.4.1.16 into Equation 6.4.1.12:
k = kBThe−ΔH‡RTeΔS‡R(6.4.1.17)
Application of the Eyring Equation
The linear form of the Eyring Equation is given below:
lnkT = −ΔH†R1T + lnkBh + ΔS‡R(6.4.1.18)
The values for ΔH‡ and ΔS‡ can be determined from kinetic data obtained from a lnkT vs. 1T plot. The Equation is a straight line with negative slope, −ΔH‡R, and a y-intercept, ΔS‡R+lnkBh.
References
Chang, Raymond. Physical Chemistry for the Biosciences. USA: University Science Books, 2005. Page 338-342.
Contributors and Attributions
Kelly Louie
6.4: Transition State Theory
7: Case Studies- Kinetics |
11307 | https://brainly.com/question/42710330 | [FREE] How does the impulse-momentum relationship relate to Newton's second law? - brainly.com
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How does the impulse-momentum relationship relate to Newton's second law?
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The impulse-momentum relationship is derived from Newton's second law. Impulse, which is the change in momentum, is closely related to the force applied to an object and the time interval over which the force is applied.
Explanation
The impulse-momentum relationship is closely related to Newton's second law. Newton's second law states that the force acting on an object is equal to the rate of change of its momentum. Mathematically, this can be represented as F = ma, where F is the force, m is the mass, and a is the acceleration. Impulse, on the other hand, is defined as the change in momentum of an object.
Impulse is equal to the force applied to an object multiplied by the time interval over which the force is applied. Mathematically, this can be represented as J = Ft, where J is the impulse, F is the force, and t is the time interval.
Therefore, the relationship between impulse and momentum can be derived from Newton's second law. Since impulse is equal to the change in momentum, the impulse-momentum relationship can be expressed as J = Δp, where J is the impulse and Δp is the change in momentum.
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The impulse-momentum relationship is derived from Newton's second law, relating the impulse (change in momentum) to the average force applied over time. Mathematically, impulse can be expressed as J=F Δ t and is equal to the change in momentum J=Δ p. This connection highlights how forces acting over time affect an object's motion.
Explanation
The impulse-momentum relationship connects closely to Newton's second law of motion, which states that the net force acting on an object is equal to the rate of change of its momentum. This can be expressed mathematically as:
F=d t d p
where F is the force, p is the momentum, and t is time.
Impulse is defined as the change in momentum resulting from a force applied over a specific time period. It can be represented mathematically as:
J=F Δ t
where J is impulse, F is the average force applied, and Δ t is the time duration over which the force is applied. The impulse experienced by an object is equal to its change in momentum:
J=Δ p
This relationship shows how when a net force acts on an object for a certain amount of time, it changes the object's momentum.
This connection means that understanding impulse helps us comprehend how forces influence the motion of objects, especially in situations with varying forces or in collisions.
To derive the impulse-momentum theorem from Newton's second law, we can integrate the force over time:
J=∫F d t=Δ p
This implies that the total impulse applied to an object equals the change in momentum of that object, thereby linking both concepts smoothly. Therefore, while Newton's second law focuses on the relation between force and motion directly, the impulse-momentum theorem emphasizes the same relation but in the context of time and change in momentum.
Examples & Evidence
A practical example of this concept is seen in sports. When a soccer player kicks a ball, the force applied to the ball (a large force) is exerted over a very short time (the duration of the kick), resulting in a significant change in the ball's momentum. In contrast, if a light breeze (a small force) were to push the same ball continuously for a longer time, it could also impart a notable change in momentum, but this would require more time compared to the kick.
Newton's second law and the concepts of impulse and momentum are foundational principles in classical mechanics, supported by extensive experimental validation and practical applications in engineering, physics, and various technologies.
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Community Answer 4 Show that the relationship between impulse and the change in momentum is another way of stating Newton's second law of motion.
Community Answer Using Newton's second law of motion explain impulse momentum principle
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Community Answer The impulse-momentum relationship is a direct result of Newton's O third law O Law of Gravity O first law O second law
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11308 | http://hyperphysics.phy-astr.gsu.edu/hbase/surten2.html | Surface Tension and BubblesThesurface tensionof water provides the necessary wall tension for the formation of bubbles with water. The tendency to minimize that wall tension pulls the bubbles into spherical shapes (LaPlace's law).Theinterference colorsindicate that the thickness of the soap film is on the order of a few wavelengths of visible light. Even though the soap film has less surface tension than pure water, which would pull itself into tiny droplets, it is nevertheless strong to be able to maintain the bubble with such a small thickness.Thepressuredifference between the inside and outside of a bubble depends upon the surface tension and the radius of the bubble. The relationship can be obtained by visualizing the bubble as two hemispheres and noting that the internal pressure which tends to push the hemispheres apart is counteracted by the surface tension acting around the cirumference of the circle.For a bubble with two surfaces providing tension, the pressure relationship is:Derive the relationshipSoap bubbles | Thesurface tensionof water provides the necessary wall tension for the formation of bubbles with water. The tendency to minimize that wall tension pulls the bubbles into spherical shapes (LaPlace's law).Theinterference colorsindicate that the thickness of the soap film is on the order of a few wavelengths of visible light. Even though the soap film has less surface tension than pure water, which would pull itself into tiny droplets, it is nevertheless strong to be able to maintain the bubble with such a small thickness. | | Derive the relationship | Soap bubbles | IndexFluid concepts
Thesurface tensionof water provides the necessary wall tension for the formation of bubbles with water. The tendency to minimize that wall tension pulls the bubbles into spherical shapes (LaPlace's law).Theinterference colorsindicate that the thickness of the soap film is on the order of a few wavelengths of visible light. Even though the soap film has less surface tension than pure water, which would pull itself into tiny droplets, it is nevertheless strong to be able to maintain the bubble with such a small thickness. |
Derive the relationship | Soap bubbles
HyperPhysicsMechanicsFluidsR Nave | HyperPhysicsMechanicsFluids | R Nave | Go Back
HyperPhysicsMechanicsFluids | R Nave
Surface Tension and Bubbles
Thesurface tensionof water provides the necessary wall tension for the formation of bubbles with water. The tendency to minimize that wall tension pulls the bubbles into spherical shapes (LaPlace's law).Theinterference colorsindicate that the thickness of the soap film is on the order of a few wavelengths of visible light. Even though the soap film has less surface tension than pure water, which would pull itself into tiny droplets, it is nevertheless strong to be able to maintain the bubble with such a small thickness. |
The surface tension of water provides the necessary wall tension for the formation of bubbles with water. The tendency to minimize that wall tension pulls the bubbles into spherical shapes (LaPlace's law).
The interference colors indicate that the thickness of the soap film is on the order of a few wavelengths of visible light. Even though the soap film has less surface tension than pure water, which would pull itself into tiny droplets, it is nevertheless strong to be able to maintain the bubble with such a small thickness.
The pressure difference between the inside and outside of a bubble depends upon the surface tension and the radius of the bubble. The relationship can be obtained by visualizing the bubble as two hemispheres and noting that the internal pressure which tends to push the hemispheres apart is counteracted by the surface tension acting around the cirumference of the circle.
For a bubble with two surfaces providing tension, the pressure relationship is:
Derive the relationship | Soap bubbles
HyperPhysicsMechanicsFluids | R Nave
Bubble PressureThe net upward force on the top hemisphere of thebubbleis just thepressuredifference times the area of the equatorial circle:The force of thesurface tensiondownward on the entire circumference of the circle is twice the surface tension times the circumference, since two surfaces contribute to the force:This givesThis latter case also applies to the case of a bubble surrounded by a liquid, such as the case of thealveoli of the lungs. | IndexFluid concepts
HyperPhysicsMechanicsFluidsR Nave | HyperPhysicsMechanicsFluids | R Nave | Go Back
HyperPhysicsMechanicsFluids | R Nave
Bubble Pressure
The net upward force on the top hemisphere of the bubble is just the pressure difference times the area of the equatorial circle:
The force of the surface tension downward on the entire circumference of the circle is twice the surface tension times the circumference, since two surfaces contribute to the force:
This gives
This latter case also applies to the case of a bubble surrounded by a liquid, such as the case of the alveoli of the lungs.
HyperPhysicsMechanicsFluids | R Nave
Surface Tension and DropletsSurface tensionis responsible for the shape of liquid droplets. Although easily deformed, droplets of water tend to be pulled into a spherical shape by thecohesiveforces of the surface layer. The spherical shape minimizes then necessary "wall tension" of the surface layer according toLaPlace's law. At left is a single early morning dewdrop in an emerging dogwood blossom.Surface tension and adhesion determine the shape of this drop on a twig. It dropped a short time later, and took a more nearly spherical shape as it fell. Falling drops take a variety of shapes due to oscillation and the effects of air friction.A water droplet can act as lens and form an image as asimple magnifier.The relatively high surface tension of water accounts for the ease with which it can be nebulized, or placed into aerosol form. Low surface tension liquids tend to evaporate quickly and are difficult to keep in an aerosol form. All liquids display surface tension to some degree. The surface tension of liquid lead is utilized to advantage in the manufacture of various sizes of lead shot. Molten lead is poured through a screen of the desired mesh size at the top of a tower. The surface tension pulls the lead into spherical balls, and it solidifies in that form before it reaches the bottom of the tower. | | Surface tensionis responsible for the shape of liquid droplets. Although easily deformed, droplets of water tend to be pulled into a spherical shape by thecohesiveforces of the surface layer. The spherical shape minimizes then necessary "wall tension" of the surface layer according toLaPlace's law. At left is a single early morning dewdrop in an emerging dogwood blossom. | Surface tension and adhesion determine the shape of this drop on a twig. It dropped a short time later, and took a more nearly spherical shape as it fell. Falling drops take a variety of shapes due to oscillation and the effects of air friction. | | IndexFluid concepts
| Surface tensionis responsible for the shape of liquid droplets. Although easily deformed, droplets of water tend to be pulled into a spherical shape by thecohesiveforces of the surface layer. The spherical shape minimizes then necessary "wall tension" of the surface layer according toLaPlace's law. At left is a single early morning dewdrop in an emerging dogwood blossom.
Surface tension and adhesion determine the shape of this drop on a twig. It dropped a short time later, and took a more nearly spherical shape as it fell. Falling drops take a variety of shapes due to oscillation and the effects of air friction. |
HyperPhysicsMechanicsFluidsR Nave | HyperPhysicsMechanicsFluids | R Nave | Go Back
HyperPhysicsMechanicsFluids | R Nave
Surface Tension and Droplets
| Surface tensionis responsible for the shape of liquid droplets. Although easily deformed, droplets of water tend to be pulled into a spherical shape by thecohesiveforces of the surface layer. The spherical shape minimizes then necessary "wall tension" of the surface layer according toLaPlace's law. At left is a single early morning dewdrop in an emerging dogwood blossom.
Surface tension is responsible for the shape of liquid droplets. Although easily deformed, droplets of water tend to be pulled into a spherical shape by the cohesive forces of the surface layer. The spherical shape minimizes then necessary "wall tension" of the surface layer according to LaPlace's law. At left is a single early morning dewdrop in an emerging dogwood blossom.
Surface tension and adhesion determine the shape of this drop on a twig. It dropped a short time later, and took a more nearly spherical shape as it fell. Falling drops take a variety of shapes due to oscillation and the effects of air friction. |
Surface tension and adhesion determine the shape of this drop on a twig. It dropped a short time later, and took a more nearly spherical shape as it fell. Falling drops take a variety of shapes due to oscillation and the effects of air friction.
A water droplet can act as lens and form an image as a simple magnifier.
The relatively high surface tension of water accounts for the ease with which it can be nebulized, or placed into aerosol form. Low surface tension liquids tend to evaporate quickly and are difficult to keep in an aerosol form. All liquids display surface tension to some degree. The surface tension of liquid lead is utilized to advantage in the manufacture of various sizes of lead shot. Molten lead is poured through a screen of the desired mesh size at the top of a tower. The surface tension pulls the lead into spherical balls, and it solidifies in that form before it reaches the bottom of the tower.
HyperPhysicsMechanicsFluids | R Nave
Capillary ActionCapillary action is the result ofadhesionandsurface tension. Adhesion of water to the walls of a vessel will cause an upward force on the liquid at the edges and result in a meniscus which turns upward. The surface tension acts to hold the surface intact, so instead of just the edges moving upward, the whole liquid surface is dragged upward. | Capillary action is the result ofadhesionandsurface tension. Adhesion of water to the walls of a vessel will cause an upward force on the liquid at the edges and result in a meniscus which turns upward. The surface tension acts to hold the surface intact, so instead of just the edges moving upward, the whole liquid surface is dragged upward. | | IndexFluid concepts
Capillary action is the result ofadhesionandsurface tension. Adhesion of water to the walls of a vessel will cause an upward force on the liquid at the edges and result in a meniscus which turns upward. The surface tension acts to hold the surface intact, so instead of just the edges moving upward, the whole liquid surface is dragged upward. |
HyperPhysicsMechanicsFluidsR Nave | HyperPhysicsMechanicsFluids | R Nave | Go Back
HyperPhysicsMechanicsFluids | R Nave
Capillary Action
Capillary action is the result ofadhesionandsurface tension. Adhesion of water to the walls of a vessel will cause an upward force on the liquid at the edges and result in a meniscus which turns upward. The surface tension acts to hold the surface intact, so instead of just the edges moving upward, the whole liquid surface is dragged upward. |
Capillary action is the result of adhesion and surface tension. Adhesion of water to the walls of a vessel will cause an upward force on the liquid at the edges and result in a meniscus which turns upward. The surface tension acts to hold the surface intact, so instead of just the edges moving upward, the whole liquid surface is dragged upward.
HyperPhysicsMechanicsFluids | R Nave
Capillary ActionCapillary actionoccurs when theadhesionto the walls is stronger than thecohesiveforces between the liquid molecules. The height to which capillary action will take water in a uniform circular tube is limited bysurface tension. Acting around the circumference, the upward force isThe height h to which capillary action will lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byShow calculation | Capillary actionoccurs when theadhesionto the walls is stronger than thecohesiveforces between the liquid molecules. The height to which capillary action will take water in a uniform circular tube is limited bysurface tension. Acting around the circumference, the upward force is | | The height h to which capillary action will lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byShow calculation | IndexFluid concepts
Capillary actionoccurs when theadhesionto the walls is stronger than thecohesiveforces between the liquid molecules. The height to which capillary action will take water in a uniform circular tube is limited bysurface tension. Acting around the circumference, the upward force is | | The height h to which capillary action will lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byShow calculation
HyperPhysicsMechanicsFluidsR Nave | HyperPhysicsMechanicsFluids | R Nave | Go Back
HyperPhysicsMechanicsFluids | R Nave
Capillary Action
Capillary actionoccurs when theadhesionto the walls is stronger than thecohesiveforces between the liquid molecules. The height to which capillary action will take water in a uniform circular tube is limited bysurface tension. Acting around the circumference, the upward force is | | The height h to which capillary action will lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byShow calculation
Capillary action occurs when the adhesion to the walls is stronger than the cohesive forces between the liquid molecules. The height to which capillary action will take water in a uniform circular tube is limited by surface tension. Acting around the circumference, the upward force is
The height h to which capillary action will lift water depends upon the weight of water which the surface tension will lift:
The height to which the liquid can be lifted is given by
HyperPhysicsMechanicsFluids | R Nave
Capillary Action CalculationThe height h to whichCapillary actionwill lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byDiscussion | | | The height h to whichCapillary actionwill lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byDiscussion | IndexFluid concepts
| | The height h to whichCapillary actionwill lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byDiscussion
HyperPhysicsMechanicsFluidsR Nave | HyperPhysicsMechanicsFluids | R Nave | Go Back
HyperPhysicsMechanicsFluids | R Nave
Capillary Action Calculation
| | The height h to whichCapillary actionwill lift water depends upon theweightof water which the surface tension will lift:The height to which the liquid can be lifted is given byDiscussion
The height h to which Capillary action will lift water depends upon the weight of water which the surface tension will lift:
The height to which the liquid can be lifted is given by
HyperPhysicsMechanicsFluids | R Nave |
11309 | https://www.sciencedirect.com/science/article/abs/pii/S0360319920336260 | A review on hydrogen generation from the hydrolysis of sodium borohydride - ScienceDirect
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International Journal of Hydrogen Energy
Volume 46, Issue 1, 1 January 2021, Pages 726-765
Review Article
A review on hydrogen generation from the hydrolysis of sodium borohydride
Author links open overlay panel Hani Nasser Abdelhamid
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Highlights
•Hydrogen generation via the hydrolysis of sodium borohydride was reviewed.
•Advantages and disadvantages of reported nanocatalysts were addressed.
•Mechanisms for the hydrolysis of NaBH 4 were proposed.
•Challenges and future prospects of nanoparticles-based catalysts were discussed.
Abstract
Hydrogen is a promising alternative energy source to conventional fuels, including fossil fuel. Thus, several methods were reported for the generation of hydrogen. This review provided a comprehensive bibliometric analysis of the publications that focus on the hydrolysis or hydrolytic dehydrogenation of sodium borohydride (NaBH 4). Surveying articles in the literature showed a promising future for this technology, although some challenges lie ahead. The process can be reversible via the regeneration of the reaction by-product (NaBO 2•2H 2 O or NaBO 2•4H 2 O). The key parameters affecting the hydrolysis reaction of aqueous NaBH 4 were also summarized. The analysis of the publications indicated that hydrogen production techniques need further investigations to be competitive and for renaissance of the current applications. This review also presented concerns behind the commercialization of the generation of hydrogen gas using the hydrolysis of NaBH 4. Several materials have been reported for hydrogen generation, but thus far, no single material can simultaneously meet all the required criteria for mobile applications. Researchers and political decision-makers should manage the progress and open new channels for commercialization purposes. The hydrolysis of NaBH 4 is promising for several applications, including material science, environmental fields, and energy-based applications.
Introduction
Thomas Young (1773–1829) defined the term “energy” as “energy is the ability to do work.” It is commonly understood that “work” means the application of effort to accomplish a task. While “power” is defined as the rate at which “work” is performed. Machines are the tools that consume energy, perform work, and provide power . Before the Industrial Revolution in the 18 th century, humans extract energy from their muscles, animals (horses, oxen, or camels), the wind (windmills and sailing ships), and water (watermills). After the invention of the engine, the human becomes in necessary demand of alternative energy sources such as fossil fuels, coal, and natural gas to accomplish their revolution. In the long term, these sources are unsustainable because they are extracted and consumed at a rate that grossly exceeds the rate at which they are produced in fossil.
Among the advanced energy technologies, hydrogen is a promising alternative source of fossil fuels . Storage of hydrogen gas can be in the form of 1) molecular hydrogen: such as in that used for pressurized vessels and liquefied hydrogen tanks; 2) in the form of atomic hydrogen including metal hydrides (MH) such as alanetes (MAlH 4) and borohydrides (MBH 4) . The production and usage of hydrogen as fuel cells can be produced from several methods . The applications of hydrogen as an energy carrier dates back to 1972 with the first published paper entitled “The Hydrogen Economy–An Ultimate Economy?” . The combustion calorific value of hydrogen (1.4×10 8 J/kg) is the highest among all fossil fuels and biofuels. As of 2019, there are at more than three models of hydrogen cars in the markets, e.g., the Toyota Mirai, the Hyundai Nexo, and the Honda Clarity . However, the development of a “Hydrogen Economy” is still in the infant stage and required further investigation to reach the maximum applicability.
Compressed hydrogen or H 2 generated using the traditional methods (e.g., such as steam reforming of hydrocarbons or coal gasification) may be suitable for large energy demand applications such as vehicle applications (>50 kW). However, these methods are unsuitable for portable devices (<100 W) on account of the lower volumetric energy density of these hydrogen sources and the absence of enough storage space in small mobile devices. Chemical hydrides, including metal–boron hydrides, ammonia borane, formic acid, hydrazine hydrate, and aromatic compounds, offer sustainable hydrogen storage systems. They can provide the requirements for industrial applications . Among these sources, sodium borohydride (NaBH 4) is promising for hydrogen generation via pyrolysis or hydrolysis [25,26]. Thus, these process can be used for proton exchange membrane fuel cells (PEMFCs) .
Section snippets
Hydrolysis of hydride for hydrogen generation
Hydrolysis of borohydride is promising for the generation of hydrogen gas. The number of publications is increased exponentially over the time (Fig.1a). Most of the published materials are scientific articles (Fig.1a). The reaction can be used for several applications, including chemistry, biomedical, engineering, materials science, and so forth. (Fig.1b). The large section of the applications of hydride hydrolysis is chemistry (Fig.1b). However, there are significant increases in other
Catalysis of the hydrolysis of NaBH 4
The self-hydrolysis reaction of NaBH 4 is exothermic and spontaneous. However, the overall conversion of NaBH 4 via the self–hydrolysis reaction at ambient condition is only 7–8% . The self–hydrolysis of NaBH 4 proceeds slowly and can be eventually discontinued . Thus, a catalyst is highly required. The reaction can be heterogeneous or homogenous (Fig.3).
The hydrolysis of NaBH 4 can be catalyzed using homogenous catalysts such as acid and metal complexes (Fig.3). Both catalysts species
Acids
The hydrolysis of NaBH 4 can be accelerated using an acid (Table 1) . The application of acid as homogenous catalysts comes back to 1953 . Acid produces a proton (H+) for catalysis and the counter–ion forming a sodium salt. Mineral acids (HCl, H 2 SO 4, HNO 3, H 3 PO 4), and carboxylic acids (HCOOH and CH 3 COOH) were examined for the hydrolysis of NaBH 4 . Acids such as HCl and H 2 SO 4, with a concentration of 3N, displayed a maximum hydrogen yield of 97% and 96%, respectively . On the
Nobel metals
Noble metals–based catalysts such as Pt , Pd , Ru , and Rh exhibited superior catalytic activity towards the hydrolysis of NaBH 4 with high hydrogen generation rates (HGR).
Ruthenium based catalysts were widely used for hydrogen generation via the hydrolysis of NaBH 4 (Table 2). Ru-based catalysts were supported in different materials such as graphite support (Ru/G) , carbon (Ru/C) , Ni foam [83,84], Al 2 O 3 , anionic resin (IRA–400) , and FeCo nanoflowers . Pure
Metal-organic frameworks (MOFs)
Metal-organic frameworks (MOFs) are hybrid porous materials consisting of inorganic and organic moieties [56,, , , , , , , , , ]. MOFs offer several advantages, including large surface area, high porosity, tunable pore size, diverse crystal structure (70,000 different structures are present in Cambridge Crystal Database, CCD), and processing into a thin film, and 3D products [58,, , , , ]. They can be used as-synthesized
Metal-free catalysts
Metal-based catalysts are effective for the hydrolysis of NaBH 4. However, they are environmentally unfriendly and costly. Thus, metal-free catalysts have been explored as an alternative to the metal-based catalyst. They can be classified into carbon-based nanomaterials, IL, and treated microalgae (Table 6).
Cellulose cotton fibers (CF) are coated with chitosan (CH) with HGR of 7760±72 mL•min−1•g−1 and E a 14.41±0.46 kJ•mol−1 (Table 6) . Protonated polyethyleneimine (PEI) microgels
Factors affecting the hydrogen generation rate
The properties of nanoparticles depends on several partmeters such as capping agents , composition, defects, synthesis procedure, etc. Several parameters may affect the hydrogen generation rate for the hydrolysis of NaBH 4. These factors belong to the reactant, catalysts, and conditions of the reaction. The following sections summarize some of the critical points of these parameters.
Outlooks and challenges
Hydrogen generation via the hydrolysis of NaBH 4 offers several advantages. It can be used for several technologies, such as a micro-scale fluidized bed reactor . NaBH 4 can be synthesized using a different method with high yield . The solubility of NaBH 4 in water is relatively low (55 g per 100 g at 25°C); thus, the hydrolysis requires more water than that needed by stoichiometry to ensure the NaBH 4 remains in solution. Although NaBH 4 has a considerably higher solubility compared to
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgment
I would thank the Ministry of Higher Education and Scientific Research (MHESR) and Assiut University, Egypt, for the support.
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### All-cellulose functional membranes for water treatment: Adsorption of metal ions and catalytic decolorization of dyes
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11310 | https://math.stackexchange.com/questions/4737988/determine-the-maximum-value-of-the-sum-s-sum-n-1-infty-fracn2n-a-1 | sequences and series - Determine the maximum value of the sum $S=\sum_{n=1}^\infty \frac{n}{2^{n}} (a_1a_2…a_n)^{1/n} $ - Mathematics Stack Exchange
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Determine the maximum value of the sum S=∑∞n=1 n 2 n(a 1 a 2…a n)1/n S=∑n=1∞n 2 n(a 1 a 2…a n)1/n
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Determine the maximum value of the sum
S=∑n=1∞n 2 n(a 1 a 2…a n)1/n S=∑n=1∞n 2 n(a 1 a 2…a n)1/n
over all sequences a k a k of non negative real numbers satisfying
∑k=1∞a k=1.∑k=1∞a k=1.
I have an idea to solve this that the product may be transformed into sum by using AM-GM inequality? If I take
a 1+a 2+…+a n n≥(a 1 a 2…a n)1/n a 1+a 2+…+a n n≥(a 1 a 2…a n)1/n
I reach to a wrong answer since all a k a k can’t be equal together so what other adjustment can be done? In a solution I got, they by default assumed it to be a GP with common ratio 1/4 1/4 and a 1=3/4 a 1=3/4 but I wonder why did they choose this only?
Attempt 2 2: If I assume it to be a GP of first term a 1=a a 1=a common r r then I get a 1−r=1 a 1−r=1 and putting this in S S, I got
S=a∑n=1∞n 2 n(1−a)n−1 2 S=a∑n=1∞n 2 n(1−a)n−1 2
Now how can I proceed (maybe through derivatives but how?)?
I’m not attaching the official solution since I want a method other than that. As mentioned above they take a=3/4 a=3/4 and r=1/4 r=1/4 arbitrarily to solve but the question is why this pair only?
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edited Jul 18, 2023 at 18:14
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1 Don't there exist solutions to the Putnam problems?Alan Chung –Alan Chung 2023-07-18 02:42:35 +00:00 Commented Jul 18, 2023 at 2:42
I got a solution but I couldn’t understand it.Maths2 –Maths2 2023-07-18 03:19:58 +00:00 Commented Jul 18, 2023 at 3:19
1 Quick beginner guide for asking a well-received question + please avoid "no clue" questions.Anne Bauval –Anne Bauval 2023-07-18 04:09:39 +00:00 Commented Jul 18, 2023 at 4:09
3 I have to admit, this problem is unreasonably closed. OP is making a genuine effort to ask a good question and included his thoughts and steps. Unfortunately, I do not have the reputation to cast reopen votes, but if anyone reading this has, consider reopening this question.user1003852 –user1003852 2023-07-18 08:29:49 +00:00 Commented Jul 18, 2023 at 8:29
2 This question in its current state indeed should be closed. If there is a specific part of the solution you cannot understand, please include that information, otherwise people will simply post the same answer over and over again, not solving your actual confusion. People are not mind-readers after all.Trebor –Trebor 2023-07-18 11:56:08 +00:00 Commented Jul 18, 2023 at 11:56
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What @Jorge wrote should be very helpful to see why we choose r=1/4 r=1/4. I will try to explain in more depth the complications your initial approach had and the motivation for choosing a geometric sequence.
Your Initial Approach
As you noted, if we try to attack the problem immediately with AM-GM, we get the following:
∑n=1∞n 2 n∏j=1 n a 1/n j≤∑n=1∞∑j=1 n n 2 n a j=∑j≥1∑n≥j 1 2 n a j=∑j≥1 2 1−j a j.(1)∑n=1∞n 2 n∏j=1 n a j 1/n≤∑n=1∞∑j=1 n n 2 n a j=∑j≥1∑n≥j 1 2 n a j=∑j≥1 2 1−j a j.(1)
However, there isn't much we can do here since all we know is ∑j≥1 a j=1∑j≥1 a j=1.
Motivation for Steps Forward
We should strive to manipulate the expression n 2 n∏n j=1 a 1/n j n 2 n∏j=1 n a j 1/n such that when AM-GM is applied, and we flip the sum for simplification ∑j≥0 a j∑j≥0 a j pops out.
If you play with the expression some before applying AM-GM, multiplying and dividing out numbers to the a j a j's, you'll see that you can affect the resulting coefficients of the a j a j's in your upper bound. So let's try to play with the coefficients in a very controlled manner using a sequence, say {r j}j≥1{r j}j≥1:
∑n=1∞n 2 n∏n k=1 r 1/n k∏j=1 n(a j r j)1/n≤∑n=1∞1 2 n∏n k=1 r 1/n k∑j=1 n a j r j=∑n=1∞∑j=1 n a j r j 2 n∏n k=1 r 1/n k∑n=1∞n 2 n∏k=1 n r k 1/n∏j=1 n(a j r j)1/n≤∑n=1∞1 2 n∏k=1 n r k 1/n∑j=1 n a j r j=∑n=1∞∑j=1 n a j r j 2 n∏k=1 n r k 1/n
.
=∑j=1∞∑n=j∞a j r j 2 n∏n k=1 r 1/n k=∑j=1∞a j r j∑n=j∞1 2 n∏n k=1 r 1/n k.(2)=∑j=1∞∑n=j∞a j r j 2 n∏k=1 n r k 1/n=∑j=1∞a j r j∑n=j∞1 2 n∏k=1 n r k 1/n.(2)
At this point this point, the only hope is if we consider {r k}k≥1{r k}k≥1 as a geometric sequence; otherwise the calculation seems intractable. Additionally, we're hinted towards this direction since we'd like the sum in n n to be a constant.
Following Through on a Hope
(After this point you could refer to Jorge's work, it is fundamentally the same.)
So let r k=r k r k=r k:
∑j=1∞a j r j−1/2∑n=j∞1 2 n r n 2=∑j=1∞a j r j−1/2 1 2 j r j/2∑n=0∞1(2 r 1/2)n=∑j=1∞a j r j−1/2 2 j r j/2 2 r 1/2 2 r 1/2−1=∑j=1∞a j r j/2 2 j−1 1 2 r 1/2−1=1 2 r 1/2−1∑j=1∞a j r j/2 2 j−1∑j=1∞a j r j−1/2∑n=j∞1 2 n r n 2=∑j=1∞a j r j−1/2 1 2 j r j/2∑n=0∞1(2 r 1/2)n=∑j=1∞a j r j−1/2 2 j r j/2 2 r 1/2 2 r 1/2−1=∑j=1∞a j r j/2 2 j−1 1 2 r 1/2−1=1 2 r 1/2−1∑j=1∞a j r j/2 2 j−1
.
Remember that we want ∑j≥1 a j∑j≥1 a j up to some constant so this means that r j/2/2 j−1 r j/2/2 j−1 needs to be a constant. We note that r 1/2/1=c r 1/2/1=c and r/2=c r/2=c; using the ratio of these two equalities, we get ⇒r 1/2=2⇒r=4⇒r 1/2=2⇒r=4.
This gives us that the sum should be bounded by 1 4−1(∑j≥1 a j)4 j/2 2 j−1=1 3(1)2 j 2 j−1=2 3 1 4−1(∑j≥1 a j)4 j/2 2 j−1=1 3(1)2 j 2 j−1=2 3.
The other half of the problem is to find a sequence which meets the upper bound. Once that is done you've shown it's the maximum.
Takeaway
My recommendation is that you write out the expanded form in columns and rows of the sum your initial approach gave you (1). Then expand the sum I give in (2). Then, if you stare at (2) expanded long enough, you'll get the impression that the problem is sort of analogous to a double-counting problem (except instead of things being overcounted, they're being undercounted); so perhaps we could use the sequence {r j}j≥1{r j}j≥1 to redress this undercounting.
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edited Jul 19, 2023 at 19:23
answered Jul 19, 2023 at 18:32
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1 Thanks now it’s perfectly clear Maths2 –Maths2 2023-07-20 02:10:22 +00:00 Commented Jul 20, 2023 at 2:10
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I have no idea how to prove that the optimal solution is geometric, but if you assume it is, you have for all n n, a n=a 1 r n−1 a n=a 1 r n−1 for some 0⩽r<1 0⩽r<1 and ∑∞n=1 a n=a 1 1−r=1∑n=1∞a n=a 1 1−r=1 hence a 1=1−r a 1=1−r. From here, you have for all n n,
n 2 n(a 1⋯a n)1/n=(1−r)n 2 n(r 0⋯r n−1)1/n=(1−r)n 2 n r(n−1)/2=1−r 2 n(r√2)n−1.n 2 n(a 1⋯a n)1/n=(1−r)n 2 n(r 0⋯r n−1)1/n=(1−r)n 2 n r(n−1)/2=1−r 2 n(r 2)n−1.
Now, use the fac that ∑n⩾1 x n=1 1−x−1∑n⩾1 x n=1 1−x−1 and differentiate this equality to deduce that ∑n⩾1 n x n−1=1(1−x)2∑n⩾1 n x n−1=1(1−x)2. Therefore,
∑n⩾1 n 2 n(a 1⋯a n)1/n=1−r 2∑n⩾1 n(r√2)n−1=1−r 2 1(1−r√2)2=2−2 r(2−r√)2.∑n⩾1 n 2 n(a 1⋯a n)1/n=1−r 2∑n⩾1 n(r 2)n−1=1−r 2 1(1−r 2)2=2−2 r(2−r)2.
It means that we must find the r r between 0 0 and 1 1 that maximizes f(r)=2−2 r(2−r√)2 f(r)=2−2 r(2−r)2. We have if 0<r<1 0<r<1,
f′(r)=−2⋅(2−r√)2−(2−2 r)⋅2−1 2 r√(2−r√)(2−r√)4=−2 r√(2−r√)+2−2 r r√(2−r√)3=2−4 r√r√(2−r√)3 f′(r)=−2⋅(2−r)2−(2−2 r)⋅2−1 2 r(2−r)(2−r)4=−2 r(2−r)+2−2 r r(2−r)3=2−4 r r(2−r)3
Therefore, f′(r)f′(r) vanishes at r=1/4 r=1/4, is positive before and negative after. We deduce that r=1/4 r=1/4 is the optimal value and in this case, the sum is f(1/4)=2−2 1 4(2−1 4√)2=2−1 2(2−1 2)2=2 3 f(1/4)=2−2 1 4(2−1 4)2=2−1 2(2−1 2)2=2 3.
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answered Jul 19, 2023 at 14:44
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Thanks a ton for your solution. I by mistake wrote the wrong answer initially.Maths2 –Maths2 2023-07-19 16:32:41 +00:00 Commented Jul 19, 2023 at 16:32
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Let S=∑∞n=1 n 2 n(∏n i=1 a i)1 n=∑∞n=1 n 2 n r i+1 2(∏n i=1 a i r i)1 n≤∑∞n=1 1 2 n r n+1 2(∑n i=1 a i r i)=S=∑n=1∞n 2 n(∏i=1 n a i)1 n=∑n=1∞n 2 n r i+1 2(∏i=1 n a i r i)1 n≤∑n=1∞1 2 n r n+1 2(∑i=1 n a i r i)==∑∞i=1∑∞n=i 1 2 n r n+1 2 a i r i=∑i=1∞∑n=i∞1 2 n r n+1 2 a i r i
Now ∑∞n=i 1 2 n r n+1 2 a i r i=a i(4 r)i 2 r 1 2∑∞n=0(r 1 2 2)n=a i r 1 2(4 r)i 2 1 1−r 1 2 2=C a i(4 r)i 2∑n=i∞1 2 n r n+1 2 a i r i=a i(4 r)i 2 r 1 2∑n=0∞(r 1 2 2)n=a i r 1 2(4 r)i 2 1 1−r 1 2 2=C a i(4 r)i 2 In order to get useful information, 4 r=1 4 r=1, because that way we can use the bound on the sum of a i a i.
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answered Jul 18, 2023 at 18:42
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So what is the maximum?user1003852 –user1003852 2023-07-19 12:44:37 +00:00 Commented Jul 19, 2023 at 12:44
Please explain that at the end what is a i a i? Shouldn’t it be evaluated in the summation? Also please elaborate a bit your last conclusion.Maths2 –Maths2 2023-07-19 13:46:42 +00:00 Commented Jul 19, 2023 at 13:46
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How to apply the definition of a derivative with a piecewise function?
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Given the function:
f(x)={x 2+1 if x≥0 x 2−1 if x<0
Question: are we justified to say that the derivative at f(0) exists? If so, what is f′(0)? And how do we justify it?
Of course I do realize that the function isn't continuous at x=0 but still since the slope near x=0 seems equal near 0+ and 0− I wondered why we can't say that f′(0)=0
What I tried is this:
f′+(0)=lim h→0+(x+h)2+1−(x 2+1)h=lim h→0+(0+h)2+1−(0 2+1)h=lim h→0+h 2 h=h=0 f_-'(0)=\lim\limits_{h \to 0-}\frac{(x+h)^2+1-(x^2+1)}{h}=\lim\limits_{h \to 0-}\frac{(0+h)^2+1-(0^2+1)}{h}=\lim\limits_{h \to 0-}\frac{h^2}{h}=h=0
My conclusion is that since both the right and left limit using the definition of the derivative exist and generate the same answer the limit exists such that f'(0)=0.
Apparently this is not true, so what is my mistake?
derivatives
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edited Nov 16, 2015 at 22:26
GambitSquared
asked Nov 16, 2015 at 15:45
GambitSquaredGambitSquared
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\endgroup
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2 \begingroup did you realised that this function isn't continuous at x=0?\endgroup –janmarqz Commented Nov 16, 2015 at 15:47
2 \begingroup To add to janmarqz, a function which is not continuous cannot be differentiated.\endgroup –Amit Saxena Commented Nov 16, 2015 at 15:51
\begingroup Why can`t you differentiate is the function isn't continuous? The values of the left and right limit of the seperate derivatives are the same...\endgroup –GambitSquared Commented Nov 16, 2015 at 15:58
\begingroup A derivative is _calulated_ by limits but that isn't its definition. The definition is an instantaneous measure of the rate of change. At a discontinuity the rate of change is infinite. So a derivative can not exist. This is, in a way, similar to evaluating a function at asingularity. 1/x simply does not exist at x = 0 even though it exists at every other point in both directions do. The derivative (rate of change) does not exist at 0, even though the calculations from opposite directions of (but not acctually _at_) zero exist.\endgroup –fleablood Commented Nov 16, 2015 at 23:04
\begingroup"The values of the left and right limit of the seperate derivatives are the same." Well, as Tim Raczkowski pointed out, they are not. The right limit is 0, but the left limit is negative infinite.\endgroup –fleablood Commented Nov 16, 2015 at 23:31
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\begingroup
Any function which is differentiable at a point x_0 must also be continuous at x_0. Since the left and right hand limits of f do not agree, your function is not continuous at 0. Therefore the derivative does not exist at 0 even though the derivative seems to be approaching the same value from both directions.
In more detail, \lim_{h\to 0^+}\frac{f(0+h)-f(0)}h=\lim_{h\to 0^+}\frac{h^2+1-1}h=\lim_{h\to 0^+}h=0.
But \lim_{h\to 0^-}\frac{f(0+h)-f(0)}h=\lim_{h\to 0^-}\frac{h^2-1-1}h=\lim_{h\to 0^-}\frac{h^2-2}h=\infty.
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edited Nov 16, 2015 at 22:03
answered Nov 16, 2015 at 15:52
Tim RaczkowskiTim Raczkowski
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\endgroup
9
\begingroup If I use the definition of the limit then the left and right limit at x=0 give the same value. So if both right and left limit give the same value, then the limit exists and thus it is also differential? Is this true?\endgroup –GambitSquared Commented Nov 16, 2015 at 18:41
\begingroup No it's not true. If you were look at f'(0) directly from the definition, you would find that it does not exist.\endgroup –Tim Raczkowski Commented Nov 16, 2015 at 18:43
\begingroup How? Using the definition, I can find a left and right side value for f`(0) which are both 0.\endgroup –GambitSquared Commented Nov 16, 2015 at 20:05
\begingroup The definition is f'(x)=\lim_{h\to 0}(f(x+h)-f(x))/h. This limit does not exist for x=0.\endgroup –Tim Raczkowski Commented Nov 16, 2015 at 20:09
\begingroup Why not? I get h^2/h which is 0\endgroup –GambitSquared Commented Nov 16, 2015 at 20:33
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\begingroup
If a function g: \Bbb R \to \Bbb R is differentiable at some point x_0 \in \Bbb R, then f is also continuous in x_0.
Now, let's consider the left- and right-sided limits of your function f at the point 0. We see that \lim_{x \to 0^+} f(x) = \lim_{x \to 0^+} (x^2 + 1) = 1 \; , and \lim_{x \to 0^-} f(x) = \lim_{x \to 0^-} (x^2 - 1) = -1 \; , which means that f is not continuous at the point 0. So f is not differentiable at the point 0 and f'(0) is not defined.
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answered Nov 16, 2015 at 15:54
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\begingroup
To be differentiable a function must be continuous. Let's go back to the definition of a derivative. _NOT_ the calculation via limits of derivatives but the _conceptual_ meaning of derivative.
"The derivative of a function of a real variable measures the sensitivity to change of a quantity (a function value or dependent variable) which is determined by another quantity (the independent variable)."
So at x = 0, the functions sensitivity to change as x decreases is infinite. The function "jumps" from value 1 to value -1 in no measurable change at all. This is infinite, huge, and unmeasurable sensitivity.
In short, no derivative can exist at x = 0.
Also your calculation is in error:
f_-'(0)=\lim\limits_{h \to 0-}\frac{(x+h)^2+1-(x^2+1)}{h}=\lim\limits_{h \to 0-}\frac{(0+h)^2+1-(0^2+1)}{h}=\lim\limits_{h \to 0-}\frac{h^2}{h}=h=0 is incorrect.
f_-'(0)=\lim\limits_{h \to 0-}\frac{f(0 -h)-f(0)}{h} =\frac{[(0+h)^2-1]-[(0^2+1)]}{h} (Note: 0 - h < 0 _BUT_ 0 \ge 0 so f(0-h) = (0-h)^2 -1 = h^2 -1 but f(0) = 0^2 + 1 = 1)
=\lim\limits_{h \to 0-}\frac{h^2-2}{h}=\lim\limits_{h \to 0-}\frac{h^2 -2}{h}=h - \frac 2 h= -\infty
Which is really much more to the point.
As one can't define a discontinuous function as _two_ different values at the discontinuity there will be one direction where \lim f(x \pm h) - f(x) will _NOT_ equal 0. If so you get \lim f(x \pm h) - f(x)/h = \text{not_zero}/0 = \pm \infty
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edited Nov 16, 2015 at 23:28
answered Nov 16, 2015 at 22:54
fleabloodfleablood
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\begingroup
You can differentiate any locally integrable function if you view it as a generalized function - in other views as a distribution. The main concept to remember is u'=\delta
where u is the standard step-function and \delta is Dirac's delta. Hence f'(x)=2x+2\delta(x).
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edited Nov 17, 2015 at 0:53
answered Nov 16, 2015 at 23:35
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Maxillary Curve is convex, Mandibular Curve is concave
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Anteroposterior Curve (of Spee)
2
Mediolateral Curve (of Wilson)
3
Apex
4
Oblique Ridge
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Terms in this set (87)
MIXED (TRANSITIONAL) DENTITION
Occurs between the ages of 6-12 years of age
When does mixed dentition begin?
Begins with the eruption of the mandibular central incisor and/or the mandibular 1st molar (which does not replace a primary tooth)
What are the four quadrants?
UR: upper right
LR: lower right
UL: upper left
LL: lower left
What are sextants?
Sextants further divide the mouth into six sections
Three on maxillary arch - 5 posterior, 6 anterior, and 5 posterior (when 3rds are present)
Three on mandibular arch - 5 posterior, 6 anterior, and 5 posterior (when 3rds are present)
Tooth functions: Incisors
bite and cut food, due to triangular form
Tooth functions: Canines
pierce or tear food due to tapered shape
Tooth functions: Premolars
assist molars in grinding food (only in permanent dentition)
Tooth functions: Molars
grind food due to large occlusal tables and prominent cusps
Primary Universal Numbering
Use #A- #T
Universal Numbering
adopted by ADA 1975
Permanent Universal numbering
Use 1-32
Palmer Tooth Notation System (bracket system)
Used by orthodontists, oral surgeons, and pedodontists
Primary - letters of the alphabet - A (nearest to arch midline) through E
Permanent - numbered 1 (nearest to arch midline) through 8
World Dental (International) Federation
FDI
Adopted by the World Health Organization
Uses two digits per tooth - First number is the quadrant (1-4 Permanent and 5-8 Primary) Second number is the tooth number (1-8 starting at midline for Permanent and 1-5 starting at midline for Primary)
Enamel
Tooth crown, hardest substance in the body (96% calcium hydroxyapatite, 4% water - produced by ameloblasts)
Dentin
Underlying enamel and cementum, 70% calcium hydroxyapatite, 18% organic matter, 12% water - produced by odontoblasts
Cementum
On the tooth root, very thin, 65% calcium hydroxyapatite, 35% organic matter, 12% water - produced by cementoblasts.
Cementoenamel junction
also known as cervical line
Pulp
soft tissue, nerves and blood vessels. Pulp cavity = Pulp Chamber = Pulp or root canal. Apical foramen @ apex. Functions: formative (dentin), nutritive, sensory, and protective (reparative dentin)
Pulp cavity
Soft tissue in the cavity or space in the center of the crown and root called the
Apical foramen
a hole near the root tip (apex). Nerves and blood vessels enter the pulp through the apical foramina
Functions of the Pulp:
Formative
odontoblasts produce dentin throughout the life of the tooth
Functions of the Pulp:Sensory
nerve endings relay the sense of pain
Functions of the Pulp:Nutritive
blood vessels transport nutrients from the bloodstream to cells of the pulp and the odontoblasts.
Functions of the Pulp:Defensive or Protective
pulp responds to injury or decay by forming reparative dentin
Clinical crown
Visible portion of the crown above the gum line
Anatomic crown
portion of the tooth covered by enamel
Yes
Can babies be born with a tooth in their mouth?
Cervical line or CEJ
Separates the anatomic crown from root
CEJ characteristics
Typically the curvature is greater on the mesial then distal and greater curve in anterior than posterior.
On proximal CEJ curves toward occlusal/incisal. On facial/lingual CEJ curves towards root apex
Periodontium
Defined as the supporting tissues of the teeth in the mouth
Periodontium includes
Alveolar Bone
Attached Gingiva
Free Gingiva
Gingival Margin
Gingival Sulcus
Interdental Papilla
Periodontal Ligament
Anterior teeth
The term labial and facial are ONLY interchangeable on which teeth?
Occlusal surface
Chewing surfaces of posterior teeth
Incisal edge
Cutting surfaces of anterior teeth
Line angle
Formed by the junction of two surfaces. Named by the two surfaces that join
Division of teeth into 3rds
3 Apical Divisions
3 Horizontal Divisions
3 Vertical Divisions
Crown-root ratio
Root length divided by crown length
Much greater in health then in disease
Start at the midline and add the quad number in front of it
How do you calculate teeth numbers with the FDI numbering system?
Quad number 5
In the FDI system, what does the 1st (UR) quadrant start on?
Morphology of anatomic crown
Many rounded elevations, ridges, depressions, and grooves
Elevations (rounded)
Ridges (linear)
Depressions
Grooves
Cusps
Linear elevation, peak, or mound on the biting surfaces
Canines and posterior teeth have from one to five cusps
Most cusps are named after the closest tooth surface or line angle
Each cusp has FOUR cusp ridges (linear prominences of enamel)
Ridges
Linear elevation tooth surface named according to its location
Marginal ridge
Borders of the enamel that form mesial or distal margins of the occlusal/lingual surfaces of the teeth
Triangular ridge
Descend from the cusp tip to the middle of the occlusal (posterior teeth)
Transverse ridge
When 2 triangular ridges join between the buccal and lingual cusps on same side. bq
Oblique Ridge
Maxillary Molars only - from DB to ML triangular ridges
Cingulum
Lingual lobe of anterior teeth, bulge at cervical third
Mamelons
3 protuberances on newly erupted incisor permanent teeth
Perikymata
numerous, minute horizontal ridges on the enamel of newly erupted permanent teeth
Central Groove
Depression running mesio-distally on the occlusal.
Pit and Fissure
Very narrow cleft at depth of any groove, usual caries beginning.
Fossa
Shallow depression or concavity. On the lingual of anterior teeth, may end in pit.
Purpose of Grooves
helps deflect food during mastication
•Developmental Grooves
Separate the tooth lobes, named according to location Central Groove Lingual Groove Buccal Groove
Triangular Development Grooves
Branch off the central groove towards the line angles. Supplemental grooves shallow branches off
What does the CEJ separate?
the anatomical crown and the root
Root Trunk
The base of the root before dividing, in multi-rooted teeth
Furcation
Where the root trunk divides (furcal region) into separate roots - space between the roots
Bifurcation
A division of the root trunk into two branches, mandibular molars and maxillary 1st premolars.
Trifurcation
A division of the root trunk into three branches, maxillary molars.
Apex
End of the root
Anteroposterior Curve (of Spee)
Maxillary curve is convex, Mandibular curve is:concave
Mediolateral Curve (of Wilson)
Maxillary Curve is convex, Mandibular Curve is concave
The Height of Contour, also known as the Crest of Curvature
is that area of the surface outline that has the maximum curvature (convexity)
All teeth contact mesially/distally except
8-#9 and #24-#25
•Contact Areas - (Proximal HOC)
More incisal or occlusally located anterior to posterior, Mesial always more incisally or occlusally located except Mandibular incisors - equal, Anterior to posterior - contact becomes larger
Diastema
space that exists between two adjacent teeth in the same arch that is not the result of missing teeth.
Benefits of proximal contact
Stabilizes the position of teeth within each arch, Contact helps to prevent food impaction which contributes to tooth decay and periodontal disease, Contact protects interdental papillae of the gingiva by diverting food buccally or lingually
Embrasures
are the open spaces between teeth and around a contact. They consist of occlusal (incisal) embrasures, buccal and lingual embrasures and gingival embrasures
Interproximal or embrasure space
filled with interdental papilla -Lingual space larger than facial
What tooth is likely to have an oblique ridge
3 (only maxillary molars!)
Central grooves run
mesial to distal
As a general rule each molar cusp forms from
one lobe
Incisors form from
four lobes (3 facial and one lingual)
Canines & Premolars form from
four lobes (3 facial lobes and one lobe per lingual cusp) or five lobes - Mandibular 2nd premolars.
Molars form from
4 or 5 lobes (one lobe per each major cusp).
Angle's Classification
First described by Edward Angle in the early 1900's
Relative alignment
each maxillary tooth is slightly distal to the corresponding mandibular tooth
Class I ideal occlusion-Horizontal overlap of anterior teeth
Incisal edges of max ant teeth overlap the mandibular teeth
Class I ideal occlusion-Vertical overlap of anterior teeth
Incisal edges of max ant teeth extend below the incisal edges of mand teeth
Class I ideal occlusion-Relationship of posterior teeth
Maxillary posterior teeth are positioned slightly buccal to the mandibular posterior teeth.
Class I ideal occlusion-Relative alignment
Vertical (long) axis midline of each maxillary tooth is slightly distal to the vertical axis of the corresponding mandibular tooth
Buccal cusps of maxillary crown are
facial to mandibular
Buccal cusps of mandibular fit into
maxillary fossae
Lingual cusps of maxillary fit into
mandibular fossa
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11315 | https://en.wikipedia.org/wiki/Activity_coefficient | Jump to content
Activity coefficient
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From Wikipedia, the free encyclopedia
Value accounting for thermodynamic non-ideality of mixtures
In thermodynamics, an activity coefficient is a factor used to account for deviation of a mixture of chemical substances from ideal behaviour. In an ideal mixture, the microscopic interactions between each pair of chemical species are the same (or macroscopically equivalent, the enthalpy change of solution and volume variation in mixing is zero) and, as a result, properties of the mixtures can be expressed directly in terms of simple concentrations or partial pressures of the substances present e.g. Raoult's law. Deviations from ideality are accommodated by modifying the concentration by an activity coefficient. Analogously, expressions involving gases can be adjusted for non-ideality by scaling partial pressures by a fugacity coefficient.
The concept of activity coefficient is closely linked to that of activity in chemistry.
Thermodynamic definition
[edit]
The chemical potential, , of a substance B in an ideal mixture of liquids or an ideal solution is given by
: ,
where μ~~o~~
B is the chemical potential of a pure substance , and is the mole fraction of the substance in the mixture.
This is generalised to include non-ideal behavior by writing
when is the activity of the substance in the mixture,
: ,
where is the activity coefficient, which may itself depend on . As approaches 1, the substance behaves as if it were ideal. For instance, if ≈ 1, then Raoult's law is accurate. For > 1 and < 1, substance B shows positive and negative deviation from Raoult's law, respectively. A positive deviation implies that substance B is more volatile.
In many cases, as goes to zero, the activity coefficient of substance B approaches a constant; this relationship is Henry's law for the solvent. These relationships are related to each other through the Gibbs–Duhem equation.
Note that in general activity coefficients are dimensionless.
In detail: Raoult's law states that the partial pressure of component B is related to its vapor pressure (saturation pressure) and its mole fraction in the liquid phase,
with the convention
In other words: Pure liquids represent the ideal case.
At infinite dilution, the activity coefficient approaches its limiting value, ∞. Comparison with Henry's law,
immediately gives
In other words: The compound shows nonideal behavior in the dilute case.
The above definition of the activity coefficient is impractical if the compound does not exist as a pure liquid. This is often the case for electrolytes or biochemical compounds. In such cases, a different definition is used that considers infinite dilution as the ideal state:
with
and
The symbol has been used here to distinguish between the two kinds of activity coefficients. Usually it is omitted, as it is clear from the context which kind is meant. But there are cases where both kinds of activity coefficients are needed and may even appear in the same equation, e.g., for solutions of salts in (water + alcohol) mixtures. This is sometimes a source of errors.
Modifying mole fractions or concentrations by activity coefficients gives the effective activities of the components, and hence allows expressions such as Raoult's law and equilibrium constants to be applied to both ideal and non-ideal mixtures.
Ionic solutions
[edit]
Knowledge of activity coefficients is particularly important in the context of electrochemistry since the behaviour of electrolyte solutions is often far from ideal, even starting at low densities due to the effects of the ionic atmosphere. Additionally, they are particularly important in the context of soil chemistry due to the low volumes of solvent and, consequently, the high concentration of electrolytes.
For solution of substances which ionize in solution the activity coefficients of the cation and anion cannot be experimentally determined independently of each other because solution properties depend on both ions. Single ion activity coefficients must be linked to the activity coefficient of the dissolved electrolyte as if undissociated. In this case a mean stoichiometric activity coefficient of the dissolved electrolyte, γ±, is used. It is called stoichiometric because it expresses both the deviation from the ideality of the solution and the incomplete ionic dissociation of the ionic compound which occurs especially with the increase of its concentration.
For a 1:1 electrolyte, such as NaCl it is given by the following:
where and are the activity coefficients of the cation and anion respectively.
More generally, the mean activity coefficient of a compound of formula is given by
The prevailing view that single ion activity coefficients are unmeasurable independently, or perhaps even physically meaningless, has its roots in the work of Guggenheim in the late 1920s. In this view, the partitioning of the physical electrochemical potentials into an activity contribution and a Galvani potential contribution is arbitrary, thus nonidealities in ion activities can be remapped to nonidealities in Galvani potential and vice versa. Nevertheless, certain products of activities (such as ) reflect a charge-neutral stoichiometry that is anyway insensitive to this partitioning, so these products are physically meaningful even if the single-ion activities are not. However, chemists have never been able to give up the idea of single ion activities, and by implication single ion activity coefficients. For example, pH is defined as the negative logarithm of the hydrogen ion activity. If the prevailing view on the physical meaning and measurability of single ion activities is correct then defining pH as the negative logarithm of the hydrogen ion activity places the quantity squarely in the unmeasurable category. Recognizing this logical difficulty, International Union of Pure and Applied Chemistry (IUPAC) states that the activity-based definition of pH is a notional definition only. Despite the prevailing negative view on the measurability of single ion coefficients, the concept of single ion activities continues to be discussed in the literature.
Experimental determination of activity coefficients
[edit]
Activity coefficients may be determined experimentally by making measurements on non-ideal mixtures. Use may be made of Raoult's law or Henry's law to provide a value for an ideal mixture against which the experimental value may be compared to obtain the activity coefficient. Other colligative properties, such as osmotic pressure may also be used.
Radiochemical methods
[edit]
Activity coefficients can be determined by radiochemical methods.
At infinite dilution
[edit]
Activity coefficients for binary mixtures are often reported at the infinite dilution of each component. Because activity coefficient models simplify at infinite dilution, such empirical values can be used to estimate interaction energies. Examples are given for water:
Binary solutions with water
| X | γx∞ (K) | γW∞ (K) |
| Ethanol | 4.3800 (283.15) | 3.2800 (298.15) |
| Acetone | | 6.0200 (307.85) |
Theoretical calculation of activity coefficients
[edit]
Activity coefficients of electrolyte solutions may be calculated theoretically, using the Debye–Hückel equation or extensions such as the Davies equation, Pitzer equations or TCPC model. Specific ion interaction theory (SIT) may also be used.
For non-electrolyte solutions correlative methods such as UNIQUAC, NRTL, MOSCED or UNIFAC may be employed, provided fitted component-specific or model parameters are available. COSMO-RS is a theoretical method which is less dependent on model parameters as required information is obtained from quantum mechanics calculations specific to each molecule (sigma profiles) combined with a statistical thermodynamics treatment of surface segments.
For uncharged species, the activity coefficient γ0 mostly follows a salting-out model:
This simple model predicts activities of many species (dissolved undissociated gases such as CO2, H2S, NH3, undissociated acids and bases) to high ionic strengths (up to 5 mol/kg). The value of the constant b for CO2 is 0.11 at 10 °C and 0.20 at 330 °C.
For water as solvent, the activity aw can be calculated using:
where ν is the number of ions produced from the dissociation of one molecule of the dissolved salt, b is the molality of the salt dissolved in water, φ is the osmotic coefficient of water, and the constant 55.51 represents the molality of water. In the above equation, the activity of a solvent (here water) is represented as inversely proportional to the number of particles of salt versus that of the solvent.
Link to ionic diameter
[edit]
The ionic activity coefficient is connected to the ionic diameter by the formula obtained from Debye–Hückel theory of electrolytes:
where A and B are constants, zi is the valence number of the ion, and I is ionic strength.
Concentrated ionic solutions
[edit]
Ionic activity coefficients can be calculated theoretically, for example by using the Debye–Hückel equation. The theoretical equation can be tested by combining the calculated single-ion activity coefficients to give mean values which can be compared to experimental values.
Stokes–Robinson model
[edit]
For concentrated ionic solutions the hydration of ions must be taken into consideration, as done by Stokes and Robinson in their hydration model from 1948. The activity coefficient of the electrolyte is split into electric and statistical components by E. Glueckauf who modifies the Robinson–Stokes model.
The statistical part includes hydration index number h, the number of ions from the dissociation and the ratio r between the apparent molar volume of the electrolyte and the molar volume of water and molality b.
Concentrated solution statistical part of the activity coefficient is:
:
The Stokes–Robinson model has been analyzed and improved by other investigators. The problem with this widely accepted idea that electrolyte activity coefficients are driven at higher concentrations by changes in hydration is that water activities are completely dependent on the concentration of the ions themselves, as imposed by a thermodynamic relationship called the Gibbs-Duhem equation. This means that the activity coefficients and the corresponding water activities are linked together fundamentally, regardless of molecular-level hypotheses. Due to this high correlation, such hypotheses are not independent enough to be satisfactorily tested.
Ion trios
[edit]
The rise in activity coefficients found with most aqueous strong electrolyte systems can be explained by increasing electrostatic repulsions between ions of the same charge which are forced together as the available space between them decreases. In this way, the initial attractions between cations and anions at the low concentrations described by Debye and Hueckel are progressively overcome. It has been proposed that these electrostatic repulsions take place predominantly through the formation of so-called ion trios in which two ions of like charge interact, on average and at distance, with the same counterion as well as with each other. This model accurately reproduces the experimental patterns of activity and osmotic coefficients exhibited by numerous 3-ion aqueous electrolyte mixtures.
Dependence on state parameters
[edit]
The derivative of an activity coefficient with respect to temperature is related to excess molar enthalpy by
Similarly, the derivative of an activity coefficient with respect to pressure can be related to excess molar volume.
Application to chemical equilibrium
[edit]
At equilibrium, the sum of the chemical potentials of the reactants is equal to the sum of the chemical potentials of the products. The Gibbs free energy change for the reactions, ΔrG, is equal to the difference between these sums and therefore, at equilibrium, is equal to zero. Thus, for an equilibrium such as
Substitute in the expressions for the chemical potential of each reactant:
Upon rearrangement this expression becomes
The sum
σμ~~o~~
S + τμ~~o~~
T − αμ~~o~~
A − βμ~~o~~
B is the standard free energy change for the reaction, .
where K is the equilibrium constant. Note that activities and equilibrium constants are dimensionless numbers.
This derivation serves two purposes. It shows the relationship between standard free energy change and equilibrium constant. It also shows that an equilibrium constant is defined as a quotient of activities. In practical terms this is inconvenient. When each activity is replaced by the product of a concentration and an activity coefficient, the equilibrium constant is defined as
where [S] denotes the concentration of S, etc. In practice equilibrium constants are determined in a medium such that the quotient of activity coefficients is constant and can be ignored, leading to the usual expression
which applies under the conditions that the activity quotient has a particular (constant) value.
References
[edit]
^ IUPAC, Compendium of Chemical Terminology, 5th ed. (the "Gold Book") (2025). Online version: (2006–) "Activity coefficient". doi:10.1351/goldbook.A00116
^ DeHoff, Robert (2018). "Thermodynamics in materials science". Entropy. 20 (7) (2nd ed.): 230–231. Bibcode:2018Entrp..20..532G. doi:10.3390/e20070532. ISBN 9780849340659. PMC 7513056. PMID 33265621.
^ Ibáñez, Jorge G.; Hernández Esparza, Margarita; Doría Serrano, Carmen; Singh, Mono Mohan (2007). Environmental Chemistry: Fundamentals. Springer. ISBN 978-0-387-26061-7.
^ Atkins, Peter; dePaula, Julio (2006). "Section 5.9, The activities of ions in solution". Physical Chemistry (8th ed.). OUP. ISBN 9780198700722.
^ Jump up to: a b Guggenheim, E. A. (1928). "The Conceptions of Electrical Potential Difference between Two Phases and the Individual Activities of Ions". The Journal of Physical Chemistry. 33 (6): 842–849. doi:10.1021/j150300a003. ISSN 0092-7325.
^ IUPAC, Compendium of Chemical Terminology, 5th ed. (the "Gold Book") (2025). Online version: (2006–) "pH". doi:10.1351/goldbook.P04524
^ Rockwood, Alan L. (2015). "Meaning and Measurability of Single-Ion Activities, the Thermodynamic Foundations of pH, and the Gibbs Free Energy for the Transfer of Ions between Dissimilar Materials". ChemPhysChem. 16 (9): 1978–1991. doi:10.1002/cphc.201500044. ISSN 1439-4235. PMC 4501315. PMID 25919971.
^ May, Peter M.; May, Eric (2024). "Ion Trios: Cause of Ion Specific Interactions in Aqueous Solutions and Path to a Better pH Definition". ACS Omega. 9 (46): 46373–46386. doi:10.1021/acsomega.4c07525. PMC 11579776.
^ Betts, R. H.; MacKenzie, Agnes N. (1952). "Radiochemical Measurements of Activity Coefficients in Mixed Electrolytes". Canadian Journal of Chemistry. 30 (2): 146–162. doi:10.1139/v52-020.
^ "Activity Coefficients at Infinite Dilution of 30 Important Components from Dortmund Data Bank". Dortmund Data Bank. DDBST GmbH. Archived from the original on 3 December 2018. Retrieved 13 December 2018.
^ King, E. L. (1964). "Book Review: Ion Association, C. W. Davies, Butterworth, Washington, D.C., 1962". Science. 143 (3601): 37. Bibcode:1964Sci...143...37D. doi:10.1126/science.143.3601.37. ISSN 0036-8075.
^ Grenthe, I.; Wanner, H. "Guidelines for the extrapolation to zero ionic strength" (PDF). Archived from the original (PDF) on 2008-12-17. Retrieved 2007-07-23.
^ Ge, Xinlei; Wang, Xidong; Zhang, Mei; Seetharaman, Seshadri (2007). "Correlation and Prediction of Activity and Osmotic Coefficients of Aqueous Electrolytes at 298.15 K by the Modified TCPC Model". Journal of Chemical & Engineering Data. 52 (2): 538–547. doi:10.1021/je060451k. ISSN 0021-9568.
^ Ge, Xinlei; Zhang, Mei; Guo, Min; Wang, Xidong (2008). "Correlation and Prediction of Thermodynamic Properties of Nonaqueous Electrolytes by the Modified TCPC Model". Journal of Chemical & Engineering Data. 53 (1): 149–159. doi:10.1021/je700446q. ISSN 0021-9568.
^ Ge, Xinlei; Zhang, Mei; Guo, Min; Wang, Xidong (2008). "Correlation and Prediction of Thermodynamic Properties of Some Complex Aqueous Electrolytes by the Modified Three-Characteristic-Parameter Correlation Model". Journal of Chemical & Engineering Data. 53 (4): 950–958. doi:10.1021/je7006499. ISSN 0021-9568.
^ Ge, Xinlei; Wang, Xidong (2009). "A Simple Two-Parameter Correlation Model for Aqueous Electrolyte Solutions across a Wide Range of Temperatures". Journal of Chemical & Engineering Data. 54 (2): 179–186. doi:10.1021/je800483q. ISSN 0021-9568.
^ "Project: Ionic Strength Corrections for Stability Constants". IUPAC. Archived from the original on 29 October 2008. Retrieved 2008-11-15.
^ Klamt, Andreas (2005). COSMO-RS from quantum chemistry to fluid phase thermodynamics and drug design (1st ed.). Amsterdam: Elsevier. ISBN 978-0-444-51994-8.
^ Jump up to: a b N. Butler, James (1998). Ionic equilibrium: solubility and pH calculations. New York, NY [u.a.]: Wiley. ISBN 9780471585268.
^ Ellis, A. J.; Golding, R. M. (1963). "The solubility of carbon dioxide above 100 degrees C in water and in sodium chloride solutions". American Journal of Science. 261 (1): 47–60. Bibcode:1963AmJS..261...47E. doi:10.2475/ajs.261.1.47. ISSN 0002-9599.
^ Stokes, R. H; Robinson, R. A (1948). "Ionic Hydration and Activity in Electrolyte Solutions". Journal of the American Chemical Society. 70 (5): 1870–1878. doi:10.1021/ja01185a065. PMID 18861802.
^ Glueckauf, E. (1955). "The influence of ionic hydration on activity coefficients in concentrated electrolyte solutions". Transactions of the Faraday Society. 51: 1235. doi:10.1039/TF9555101235.
^ Glueckauf, E. (1957). "The influence of ionic hydration on activity coefficients in concentrated electrolyte solutions". Transactions of the Faraday Society. 53: 305. doi:10.1039/TF9575300305.
^ Kortüm, G. (1959). "The Structure of Electrolytic Solutions". Angewandte Chemie. 72 (24). London: Herausgeg. von W. J. Hamer; John Wiley & Sons, Inc., New York; Chapman & Hall, Ltd.: 97. doi:10.1002/ange.19600722427. ISSN 0044-8249.
^ Miller, Donald G. (1956). "On the Stokes-Robinson Hydration Model for Solutions". The Journal of Physical Chemistry. 60 (9): 1296–1299. doi:10.1021/j150543a034.
^ Nesbitt, H. Wayne (1982). "The stokes and robinson hydration theory: A modification with application to concentrated electrolyte solutions". Journal of Solution Chemistry. 11 (6): 415–422. doi:10.1007/BF00649040. S2CID 94189765.
^ May, Peter M.; May, Eric (2024). "Ion Trios: Cause of Ion Specific Interactions in Aqueous Solutions and Path to a Better pH Definition". ACS Omega. 9 (46): 46373–46386. doi:10.1021/acsomega.4c07525. PMC 11579776.
External links
[edit]
AIOMFAC online-model An interactive group-contribution model for the calculation of activity coefficients in organic–inorganic mixtures.
Electrochimica Acta Single-ion activity coefficients
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11316 | https://www.sciencedirect.com/science/article/abs/pii/S0304885323002433 | Skip to article
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Cited by (2)
Journal of Magnetism and Magnetic Materials
Volume 572, 15 April 2023, 170594
Dzyaloshinskii-Moriya interaction and skyrmions in antiferromagnetic-based heterostructures
Author links open overlay panel, , , , , , , , , , , ,
rights and content
Highlights
¢
A systematic study on the magnetic properties is carried out by first-principles calculation.
¢
The MgO/IrMn heterostructure gives rise to the large PMA and interfacial DMI.
¢
The antiferromagnetic skyrmions can be induced without any external magnetic fields.
Abstract
The Dzyaloshinskii-Moriya interaction (DMI), an antisymmetric exchange format, plays a key role in the formation of chiral magnetic states. Here, a systematic study on the magnetic properties, including DMI, Heisenberg exchange coupling, and magnetocrystalline anisotropy of IrMn (PtMn) and MgO/IrMn (MgO/PtMn) stacks were carried out by first-principles calculation. Furthermore, the effect of DMI on topological magnetism in the above structures was investigated by micromagnetic simulations based on magnetic parameters from first-principles calculation. A large DMI and microscopic mechanisms of DMI at MgO/IrMn interface were unveiled. This interfacial DMI originates from the dominant contribution from the Ir layer and the orbital hybridization with Ir 3d orbit. The micromagnetic simulation indicates that the labyrinth domains with chiral domain walls and antiferromagnetic skyrmions appear for MgO/IrMn heterostructure, and isolated antiferromagnetic skyrmions are induced for MgO/PtMn heterostructure without any external magnetic fields. Our results may open up a new route to generate the magnetic antiferromagnetic skyrmions at oxide/antiferromagnetic interfaces, which can be an ideal information carrier.
Introduction
Antiferromagnetic (AFM) materials have drawn considerable attention due to their insensitivity to external magnetic fields and zero stray magnetic fields, which can be extended to low dimensions and widespread availability used in nature with high Néel temperatures , , . In addition, the typical resonance frequency of AFM materials locates at terahertz (THz) due to strong AFM exchange interaction , and the low-energy dynamics of AFM can be regarded as solid-body rotation of the system of magnetic vectors, which can greatly simplify the description of the low-lying excitations in AFM and their interaction with external fields . The spin-valve-like magnetoresistance effect of antiferromagnetic tunnel junctions marks the formal emergence of antiferromagnetic spintronics . Furthermore, room temperature antiferromagnetic memory resistor and magnetic phase transition controlled by strain and electric fields provide further opportunities in the applications of antiferromagnetic spintronics . The realization of reversible electrical switching of antiferromagnets paves the way for antiferromagnetic information storage techniques. Recently, antiferromagnets have inspired a new field and exhibit a variety of interesting phenomena, such as the large anomalous Hall effect , , spin Hall magnetoresistance effect , , and magnetic skyrmions , , , . Although it is a great challenge to have a direct observation for antiferromagnets due to zero net magnetic moments, recent progress has shown that AFM materials play a more and more important role in spintronic applications, such as non-volatile memory , and magnetic field probes .
As mentioned above, AFM materials with weak ferromagnetism exhibit the dynamics of the domain walls and provide another opportunity to explore topological chiral spin configuration, e.g., skyrmions and spin spirals, which are widely found in noncentrosymmetric materials . Unfortunately, non-centrosymmetric magnetic crystals are considerably limited in nature. Recently, stable skyrmions and Néel-type domain walls have been found in the heavy metal/ferromagnet (HM/FM) heterostructures with strong interfacial Dzyaloshinskii-Moriya interaction (DMI) originating from spin-orbit coupling (SOC) , , . Similar to HM/FM heterostructures, a large DMI through the Fert-Levy mechanism , exists in two-dimensional (2D) magnets with a Janus structure . For the HM/AFM interface, the field-free switching of magnetization through spinorbit torque has been achieved as well , , where the interfacial DMI can be enhanced by increasing IrMn thickness . For oxide/AFM heterostructures, the most focus was given to the magnetic control of antiferromagnets such as NiFe/IrMn/MgO/Pt system . Few studies on DMI across the oxide/AFM interface and its effect on the topological state has been reported. The AFM materials such as IrMn and PtMn are attracting more and more attention due to the maximization of magnetic anisotropy in bimetallic systems by combining large spontaneous magnetic moments of 3d transition metals with large magnetic susceptibility and spinorbit coupling on 5d shell of noble metals . In addition, both IrMn and PtMn have high Néel temperatures (975 K and 1145 K), which attract considerable attention as a good stabilizable antiferromagnetic layer , .
In this work, a systematic study of the magnetic properties, including DMI, Heisenberg exchange coupling, and magnetocrystalline anisotropy of IrMn (PtMn) and MgO/IrMn (MgO/PtMn) stacks were carried out by the first-principles calculation, as well as a further investigation on the topological magnetism by micromagnetic simulation. It is found that MgO/IrMn interface gives rise to a large PMA and reduces Heisenberg exchange coupling. Meanwhile, the interfacial DMI (iDMI) is greatly enhanced due to the Ir layer and the orbital hybridization with Ir 3d orbit. A detailed analysis of the spin-orbital coupling energy contribution of the DMI from IrMn in comparison to the MgO/IrMn provides physical insights into the origin of the DMI. The topological magnetism in MgO/IrMn (MgO/PtMn) stacks is investigated by micromagnetic simulation based on magnetic parameters from the first-principles calculation, where the labyrinth domains with chiral domain walls and AFM skyrmions appear for MgO/IrMn stack and the AFM skyrmions are induced for MgO/PtMn stack in absence of magnetic fields.
Section snippets
Computational methods and details
The first-principles calculation was performed within the framework of density-functional theory (DFT) as implemented in the Vienna ab initio simulation package (VASP) , , . The electron-core interaction is described by the projected augmented wave (PAW) method for the pseudopotentials and the exchangecorrelation energy is included with the generalized gradient approximation (GGA) parameterized by Perdew-Burke-Ernzerhof (PBE) form . The cutoff energy for the plane-wave
Results and discussion
The () supercells of pristine IrMn, the lattice constant is 2.668 Ã
, and the IrMn under different tensile strains are investigated. The tensile strains are 1.2, 4.9, 8.7 and 11.6%. Firstly, based on the recipe of the second-order perturbation theory by Wang et al. , the MAE is defined as the energy difference between the out-of-plane and in-plane magnetizations, where the positive and negative values represent the perpendicular magnetic anisotropy (PMA) and in-plane magnetic anisotropy
Conclusions
In summary, using first-principles calculation and micromagnetic simulation, it is found that the magnetization orients change from in-plane to out-of-plane by depositing IrMn (PtMn) on MgO substrate and a large DMI exists at MgO/IrMn interface. Further, the main features and microscopic mechanisms of large DMI were unveiled. Furthermore, the labyrinth domains with chiral domain walls and antiferromagnetic skyrmions exist for MgO/IrMn and the stable antiferromagnetic skyrmions can be induced
CRediT authorship contribution statement
Y.Q. Guo: Conceptualization, Methodology, Visualization, Investigation, Writing review & editing. P. Li: Methodology, Validation. Q.R. Cui: Validation. Y.L. Ga: Methodology, Validation. L.M. Wang: Validation. H.X. Yang: Methodology, Resources, Funding acquisition, Writing review & editing. J.J. Zhou: Investigation. T. Zhu: Supervision, Funding acquisition. C.Q. Hu: Investigation. Y. Gao: Investigation. C.L. He: Supervision. S.P. Shen: Supervision. S.G. Wang: Conceptualization, Resources,
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
This work was supported by the National Key R&D plan program of China (Grant No. 2021YFA1400300) and the National Natural Science Foundation of China (Grant Nos. 51901025, 11904025, and 52130103).
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Cited by (2)
Tailoring bimeron-antibimeron in Permalloy submicron dot via fieldinduced magnetization reversal
2025, Results in Surfaces and Interfaces
The controlled nucleation and manipulation of topological spin textures such as bimerons and antibimerons, remain significant challenges for advancing spintronic technologies. We investigate the tunable controllability and selective manipulation of bimeron and antibimeron pairs in two thicknesses (t = 2 and 4 nm) of Py sub-micron dot systems using magnetization reversal investigation in micromagnetic simulations. By systematically varying material parameters such as the DzyaloshinskiiMoriya interaction (DMI) constant, dot thickness, and applying external bias fields, we demonstrate control over the nucleation, stability, and annihilation of bimeron-antibimeron pairs. Our results reveal that the size of the bimeronantibimeron pair approximately reduces from 23 to 19 nm when the thickness of the dot is increased from 2 to 4 nm. It is also seen that the spatial separation of bimeron pairs is strongly dependent on the dot thickness. Notably, the selective stabilization of either bimerons or antibimerons can be achieved by adjusting the sign and magnitude of the DMI constant (D = ±3.0 mJ/m2). Finally, the application of suitable bias fields during magnetization reversal enables additional selectivity in controlling these topological spin textures. These findings provide new insights into the engineering and manipulation of topologically protected bimerons-antibimerons spin textures, highlighting their potential for future spintronic device applications.
### Nonreciprocal Spin Cherenkov excitation induced by Dzyaloshinskii-Moriya interaction in ferromagnetic nanowires
2025, Physica B Condensed Matter
The Spin-Cherenkov Effect (SCE) is a spin wave (SW) excitation phenomenon that occurs when a disturbance in the magnetic system exceeds the minimum phase velocity of the SWs. In this study, we investigate the influence of bulk Dzyaloshinskii-Moriya interaction (DMI), an antisymmetric exchange interaction, on the SCE in quasi-three-dimensional permalloy nanostrips using micromagnetic simulations. Our results show that the SWs excited by moving magnetic pulses in the system exhibit notable nonreciprocity that is dependent on the strength of the bulk DMI. Furthermore, we demonstrate that applying a spin-polarized electric current can effectively manipulate this nonreciprocity. Analytical calculations accounting for the bulk DMI and spin transfer torque are in good agreement with our numerical results. The combination of DMI and an electric current provides an effective means for harnessing the nonreciprocal Cherenkov excitation of SWs, which may have potential applications in the development of magnonic devices.
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References
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Weiss KH, Gotthardt DN, Klemm D, et al. Zinc monotherapy is not as effective as chelating agents in treatment of Wilson disease. Gastroenterology. 2011 Apr. 140(4):1189-98.e1. [QxMD MEDLINE Link].
da Costa Mdo D, Spitz M, Bacheschi LA, Leite CC, Lucato LT, Barbosa ER. Wilson's disease: two treatment modalities. Correlations to pretreatment and posttreatment brain MRI. Neuroradiology. 2009 Oct. 51(10):627-33. [QxMD MEDLINE Link].
Brewer GJ, Askari F, Dick RB, et al. Treatment of Wilson's disease with tetrathiomolybdate: V. control of free copper by tetrathiomolybdate and a comparison with trientine. Transl Res. 2009 Aug. 154(2):70-7. [QxMD MEDLINE Link].
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Gerosa C, Fanni D, Congiu T, et al. Liver pathology in Wilson's disease: from copper overload to cirrhosis. J Inorg Biochem. 2019 Jan 15. 193:106-11. [QxMD MEDLINE Link].
Schilsky ML, Czlonkowska A, Zuin M, et al, for the CHELATE trial investigators. Trientine tetrahydrochloride versus penicillamine for maintenance therapy in Wilson disease (CHELATE): a randomised, open-label, non-inferiority, phase 3 trial. Lancet Gastroenterol Hepatol. 2022 Dec. 7 (12):1092-102. [QxMD MEDLINE Link].
Tables
| | | | | | |
--- --- --- |
| Score | 0 | 1 | 2 | 3 | 4 |
| Serum bilirubin (reference range, 3-20 mmol/L) | < 100 | 100-150 | 151-200 | 201-300 | >300 |
| Serum aspartate transaminase (reference range, 7-40 IU/L) | < 100 | 100-150 | 151-200 | 201-300 | >300 |
| Prothrombin time prolongation (seconds) | < 4 | 4-8 | 9-12 | 13-20 | >30 |
Score
0
1
2
3
4
Serum bilirubin (reference range, 3-20 mmol/L)
< 100
100-150
151-200
201-300
300
Serum aspartate transaminase (reference range, 7-40 IU/L)
< 100
100-150
151-200
201-300
300
Prothrombin time prolongation (seconds)
< 4
4-8
9-12
13-20
30
Contributor Information and Disclosures
Richard K Gilroy, MD, FRACP Gastroenterologist, Intermountain Healthcare
Disclosure: Received salary from gilead, NPS pharmaceuticals, salix pharmaceuticals, AbbVie for speaking and teaching.
Rahil Shah, MD Consulting Staff, Lebanon Endoscopy Center
Rahil Shah, MD is a member of the following medical societies: American College of Gastroenterology, American Society for Gastrointestinal Endoscopy
Disclosure: Received consulting fee from Takeda for speaking and teaching.
Michael H Piper, MD Clinical Assistant Professor, Department of Internal Medicine, Division of Gastroenterology, Wayne State University School of Medicine; Consulting Staff, Digestive Health Associates, PLC
Michael H Piper, MD is a member of the following medical societies: Alpha Omega Alpha, American College of Gastroenterology, American College of Physicians, Michigan State Medical Society
Disclosure: Nothing to disclose.
Praveen K Roy, MD, MSc Clinical Assistant Professor of Medicine, University of New Mexico School of Medicine
Praveen K Roy, MD, MSc is a member of the following medical societies: Alaska State Medical Association, American Gastroenterological Association
Disclosure: Nothing to disclose.
Erawati V Bawle, MD, FAAP, FACMG Retired Professor, Department of Pediatrics, Wayne State University School of Medicine
Erawati V Bawle, MD, FAAP, FACMG is a member of the following medical societies: American College of Medical Genetics and American Society of Human Genetics
Disclosure: Nothing to disclose.
Selim R Benbadis, MD Professor, Director of Comprehensive Epilepsy Program, Departments of Neurology and Neurosurgery, Tampa General Hospital, University of South Florida College of Medicine
Selim R Benbadis, MD is a member of the following medical societies: American Academy of Neurology, American Academy of Sleep Medicine, American Clinical Neurophysiology Society, American Epilepsy Society, and American Medical Association
Disclosure: UCB Pharma Honoraria Speaking, consulting; Lundbeck Honoraria Speaking, consulting; Cyberonics Honoraria Speaking, consulting; Glaxo Smith Kline Honoraria Speaking, consulting; Sleepmed/DigiTrace Honoraria Speaking, consulting; Sunovion Consulting fee None
Bruce Buehler, MD Professor, Department of Pediatrics and Genetics, Director RSA, University of Nebraska Medical Center
Bruce Buehler, MD is a member of the following medical societies: American Academy for Cerebral Palsy and Developmental Medicine, American Academy of Pediatrics, American Association on Mental Retardation, American College of Medical Genetics, American College of Physician Executives, American Medical Association, and Nebraska Medical Association
Disclosure: Nothing to disclose.
Beth A Carter, MD Assistant Professor of Pediatrics, Department of Pediatric Gastroenterology, Hepatology and Nutrition, Baylor College of Medicine; Medical Director, Pediatric Intestinal Rehabilitation Program, Texas Children's Hospital
Beth A Carter, MD is a member of the following medical societies: American Gastroenterological Association, American Liver Foundation, and North American Society for Pediatric Gastroenterology, Hepatology and Nutrition
Disclosure: Nothing to disclose.
Celia H Chang, MD Health Sciences Clinical Professor, Chief, Division of Child Neurology, Department of Neurology/MIND Institute, University of California, Davis, School of Medicine
Celia H Chang is a member of the following medical societies: American Academy of Neurology and Child Neurology Society
Disclosure: Nothing to disclose.
Robert J Fingerote, MD, MSc, FRCPC Consultant, Clinical Evaluation Division, Biologic and Gene Therapies, Directorate Health Canada; Consulting Staff, Department of Medicine, Division of Gastroenterology, York Central Hospital, Ontario
Robert J Fingerote, MD, MSc, FRCPC is a member of the following medical societies: American Association for the Study of Liver Diseases, American Gastroenterological Association, Canadian Medical Association, Ontario Medical Association, and Royal College of Physicians and Surgeons of Canada
Disclosure: Nothing to disclose.
Nestor Galvez-Jimenez, MD, MSc, MHA Chairman, Department of Neurology, Program Director, Movement Disorders, Department of Neurology, Division of Medicine, Cleveland Clinic Florida
Nestor Galvez-Jimenez, MD, MSc, MHA is a member of the following medical societies: American Academy of Neurology, American College of Physicians, and Movement Disorders Society
Disclosure: Nothing to disclose.
Christopher Luzzio, MD Clinical Assistant Professor, Department of Neurology, University of Wisconsin at Madison School of Medicine and Public Health
Christopher Luzzio, MD is a member of the following medical societies: American Academy of Neurology
Disclosure: Nothing to disclose.
Francisco Talavera, PharmD, PhD Adjunct Assistant Professor, University of Nebraska Medical Center College of Pharmacy; Editor-in-Chief, Medscape Drug Reference
Disclosure: Medscape Salary Employment
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11318 | https://academic.oup.com/jid/article/231/6/e1151/8093470 | Age-Dependent Assortativeness in Herpes Simplex Virus Type 1 Oral Transmission in the United States: A Mathematical Modeling Analysis | The Journal of Infectious Diseases | Oxford Academic
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Volume 231 Issue 6 15 June 2025
Article Contents
Abstract
METHODS
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RESULTS
DISCUSSION
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Journal Article
Age-Dependent Assortativeness in Herpes Simplex Virus Type 1 Oral Transmission in the United States: A Mathematical Modeling Analysis Open Access
Hassan Hachem,
Hassan Hachem
Infectious Disease Epidemiology Group, Weill Cornell Medicine–Qatar, Cornell University, Qatar Foundation–Education City
,
Doha
,
Qatar
Department of Healthcare Policy and Research, Weill Cornell Medicine, Cornell University
,
New York, New York
,
USA
Correspondence: Laith J. Abu-Raddad, PhD, Infectious Disease Epidemiology Group, Weill Cornell Medicine–Qatar, Qatar Foundation–Education City, PO Box 24144, Doha, Qatar (lja2002@qatar-med.cornell.edu); Hassan Hachem, PhD, Infectious Disease Epidemiology Group, Weill Cornell Medicine–Qatar, Qatar Foundation–Education City, PO Box 24144, Doha, Qatar (hah4018@qatar-med.cornell.edu).
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Houssein H Ayoub,
Houssein H Ayoub
Mathematics Program, Department of Mathematics and Statistics, College of Arts and Sciences, Qatar University
,
Doha
,
Qatar
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Laith J Abu-Raddad
Laith J Abu-Raddad
Infectious Disease Epidemiology Group, Weill Cornell Medicine–Qatar, Cornell University, Qatar Foundation–Education City
,
Doha
,
Qatar
Department of Healthcare Policy and Research, Weill Cornell Medicine, Cornell University
,
New York, New York
,
USA
Department of Public Health, College of Health Sciences, QU Health, Qatar University
,
Doha
,
Qatar
College of Health and Life Sciences, Hamad bin Khalifa University
,
Doha
,
Qatar
Correspondence: Laith J. Abu-Raddad, PhD, Infectious Disease Epidemiology Group, Weill Cornell Medicine–Qatar, Qatar Foundation–Education City, PO Box 24144, Doha, Qatar (lja2002@qatar-med.cornell.edu); Hassan Hachem, PhD, Infectious Disease Epidemiology Group, Weill Cornell Medicine–Qatar, Qatar Foundation–Education City, PO Box 24144, Doha, Qatar (hah4018@qatar-med.cornell.edu).
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Potential conflicts of interest. All authors: No reported conflicts.
All authors have submitted the ICMJE Form for Disclosure of Potential Conflicts of Interest. Conflicts that the editors consider relevant to the content of the manuscript have been disclosed.
Author Notes
The Journal of Infectious Diseases, Volume 231, Issue 6, 15 June 2025, Pages e1151–e1159,
Published:
26 March 2025
Article history
Received:
09 January 2025
Editorial decision:
21 March 2025
Accepted:
22 March 2025
Published:
26 March 2025
Corrected and typeset:
10 April 2025
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Hassan Hachem, Houssein H Ayoub, Laith J Abu-Raddad, Age-Dependent Assortativeness in Herpes Simplex Virus Type 1 Oral Transmission in the United States: A Mathematical Modeling Analysis, The Journal of Infectious Diseases, Volume 231, Issue 6, 15 June 2025, Pages e1151–e1159, Select Format Download citation Close
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Abstract
Background
Herpes simplex virus type 1 (HSV-1) is a highly infectious, globally prevalent lifelong infection. Despite advancements in understanding its epidemiology, the assortativeness in the age-dependent transmission patterns remains unclear. This study aimed to estimate the degree of assortativeness in age group mixing for oral-to-oral HSV-1 transmission within the United States (US) population.
Methods
An age-structured mathematical model was employed to describe HSV-1 transmission dynamics in the US population, incorporating its different modes of transmission. The model was fitted to nationally representative HSV-1 data from the National Health and Nutrition Examination Survey (NHANES) spanning 1976–2016 using a Bayesian inference framework. The degree of assortativeness in age group mixing was calibrated on a scale from 0 (no age group bias in close-proximity interactions) to 1 (exclusive mixing within the same age group).
Results
The model demonstrated robust fits to US demographics, age-specific HSV-1 prevalence, and temporal trends in both HSV-1 prevalence and ever-symptomatic HSV-1 genital herpes prevalence. The degree of assortativeness was estimated as 0.87 (95% credible interval [CrI], .64–.99) for children, indicating strong age-based assortativity, and as 0.04 (95% CrI, .004–.10) for adults, indicating weak age-based assortativity.
Conclusions
Most HSV-1 infections among children are acquired from peers within their own age group, whereas adults acquire HSV-1 infections from a broad range of age groups.
oral herpes, genital herpes, assortativeness, Bayesian framework, mathematical model
Topic:
genital herpes
adult
child
human herpesvirus 1
infections
national health and nutrition examination survey
mathematical model
Issue Section:
Major Article>Viruses
Herpes simplex virus type 1 (HSV-1) is a highly infectious and globally prevalent lifelong infection, typically acquired during childhood [1–3]. The World Health Organization estimated that in 2020, 122.2 million new HSV-1 infections occurred worldwide among individuals aged 0–49 years, contributing to 3779.1 million prevalent infections and a global prevalence of 58.6% in this age group . HSV-1 infection is characterized by frequent subclinical infectious shedding and symptomatic reactivation in a subset of infected individuals [4–6].
The virus is primarily transmitted through contact with cold sores or oral secretions during asymptomatic shedding [5, 7, 8]. This can occur through practices that are particularly common among children, such as sharing utensils, cups, bottles, or food; kissing and other close face-to-face interactions; chewing on shared objects such as toys; and sharing personal items like toothbrushes or lip balm [5, 7, 8].
While symptomatic infection often manifests as oral or facial lesions [9, 10], HSV-1 infection can also cause a wide range of clinical presentations, including herpetic whitlow, gingivostomatitis, meningitis, encephalitis, and corneal blindness [11–13]. The virus can also be transmitted through oral sex or sexual intercourse, resulting in genital herpes infection; however, prior oral HSV-1 infection substantially reduces the risk of acquiring genital HSV-1 [8, 14, 15]. In many high-income countries, improved hygiene and living conditions have reduced the prevalence of oral infections during childhood [3, 8, 16–19], contributing to an increasing trend in the sexual acquisition of HSV-1 [8, 20–23].
Despite advancements in understanding the global epidemiology of HSV-1 infection [8, 20–27], important knowledge gaps persist. One key gap is the limited understanding of the transmission patterns of infection across different age groups. For instance, to what extent do new infections in a specific age group, such as children aged 10–14 years, result from transmission within the same age group versus from other age groups in the population?
This study aims to address this question by estimating the degree of assortativeness in age group mixing for oral-to-oral HSV-1 transmission. A mathematical model of HSV-1 transmission dynamics was employed and calibrated to the United States (US) population—the only country with repeated, nationally representative population-based surveys spanning several decades [3, 16, 28–32], enabling such an analysis. The model was used to describe HSV-1 transmission dynamics across its various modes of transmission and to estimate the degree of assortativeness in age group mixing for both children and adults, accounting for the fact that these groups may have distinct structures of social networks through which the infection is acquired.
METHODS
Mathematical Model
The study utilized a deterministic population-level dynamical model previously developed to describe oral and sexual HSV-1 transmission within a given population . The details of the model's structure, equations, and parameterization have been published elsewhere but are briefly summarized here.
The model was constructed based on the current understanding of the natural history and epidemiology of HSV-1 infection [4–6, 8, 33]. It consisted of a set of coupled nonlinear differential equations that stratified the population into compartments based on age, HSV-1 status, stage of infection, and level of oral or genital exposure risk to the infection . Model implementation and analysis were conducted using MATLAB R2019a.
The model accounted for differences in the natural history of HSV-1 infection depending on the route of exposure (oral vs genital) [4–6, 8, 33] and included 2 stages of viral shedding—primary infection and reactivation—as well as periods of latency without viral shedding between reactivation episodes . Susceptible individuals who acquired HSV-1 for the first time progressed through a primary infection phase, followed by a latent infection phase with episodic reactivations throughout their lifetime [4–6, 8, 33].
The population was stratified into 20 age groups, each representing a 5-year age band (0–4, 5–9, …, 95–99 years) . The model accounted for heterogeneity in sexual behaviors across these age groups .
Force of Infection
The force of infection in the model captures 4 distinct age-dependent transmission modes, reflecting the evolving dynamics of HSV-1 epidemiology . Infection acquisition is categorized into 2 primary pathways: oral and genital acquisition. Oral HSV-1 acquisition occurs primarily through oral-to-oral transmission, the dominant mode of infection. A small proportion of oral infections also result from genital-to-oral transmission via oral sex, though this contributes minimally to overall oral HSV-1 acquisition.
Genital HSV-1 acquisition occurs through oral-to-genital and genital-to-genital transmission. Oral-to-genital transmission, through oral sex, accounts for most new genital HSV-1 infections. Meanwhile, genital-to-genital transmission via sexual intercourse serves as a secondary mode of HSV-1 genital acquisition.
The model assumes that children aged <15 years acquire HSV-1 exclusively through oral-to-oral transmission. However, among adolescents and adults (≥15 years), all 4 transmission modes contribute to HSV-1 epidemiology. By incorporating age-dependent variations in transmission risk and behavioral heterogeneity in sexual exposure, the model provides a nuanced representation of HSV-1 transmission dynamics across different life stages.
Age Group Mixing
The mixing between populations in different age groups—representing the sociophysical interactions that facilitate oral-to-oral transmission of the infection—was characterized using a mixing matrix . This matrix defines the probability of an individual in a specific age group interacting with an individual in another age group [8, 34–36].
The matrix is structured to include 2 components: the first represents strictly assortative mixing, where interactions occur only within the same age group, while the second represents proportionate mixing, where individuals mix with others in the population without preferential bias for a specific age group [8, 34–36]. Proportionate mixing assumes that contact rates between groups are proportional to their relative sizes, resulting in random, homogeneous interactions across the entire population [8, 34–36]. This formulation provides a flexible representation of real-world mixing patterns, balancing age-assortative interactions with broader population-wide exposure.
The matrix is expressed as follows [8, 34–36]:
𝓗 H a,b O r a l=ε a O r a l δ a,b+(1−ε a O r a l)∑i=1 n P o p(ρ X b i O r a l X b i)∑u=1 20∑i=1 n P o p(ρ X u i O r a l X u i)
Here, a indexes the 20 age groups in the model, and i indexes the different population variables (X a i) in the model. δ a,b represents the identity matrix, and ρ X a i O r a l is the sociophysical contact rate for the X a i population. The parameter ε a O r a l represents the degree of assortativeness in age group mixing and is defined as:
ε a O r a l={ε c h i l d h o o d if a<15 years age ε a d u l t h o o d if a≥15 years age
Accordingly, there are 2 assortativeness parameters estimated in this study: one for children and one for adults.
This form of the mixing matrix accommodates a spectrum of mixing behaviors, ranging from fully assortative mixing to fully proportionate mixing [8, 34–36]. At one extreme, where ε a O r a l=1, mixing is fully assortative, indicating that individuals interact exclusively within their own age group [8, 34–36]. Conversely, at the other extreme, ε a O r a l=0, mixing is fully proportionate, signifying no preferential bias in age group interactions [8, 34–36].
Notably, while this formulation of the mixing matrix is flexible and accommodates diverse mixing patterns, it is not exhaustive and does not account for all theoretically possible interactions. Further details on the mixing matrix structure, population variables, and definitions can be found in Ayoub et al .
Data Sources and Model Parameters
The model parameter values were derived from primary studies on HSV-1 natural history, epidemiology, and reported sexual behavior patterns, as detailed previously, including the parameter values, their justifications, and sources . Demographic data, including population size by age, as well as historical and future projections, were obtained from the Population Division database of the United Nations Department of Economic and Social Affairs .
A range of epidemiological data was derived from 11 publicly available biennial rounds of the National Health and Nutrition Examination Survey (NHANES), conducted between 1976 and 2016, a nationally representative and population-based survey [3, 16, 28–32]. These data were used to inform model parameters and calibrate the model. Each survey round employed standardized methodologies for both analytical and laboratory procedures [3, 16, 28–32]. Demographic, sexual behavior, and HSV-1 laboratory testing data from each round were extracted, merged, and analyzed in accordance with NHANES standardized guidelines .
The laboratory methods distinguished HSV-1 from herpes simplex virus type 2 (HSV-2) antibodies using type-specific serological testing, which detected antibodies against glycoprotein G-1 (gG-1) for HSV-1 and glycoprotein G-2 (gG-2) for HSV-2, ensuring accurate differentiation between the 2 infections. Sampling weights were applied to all NHANES-derived measures to ensure representativeness of the US population.
For each NHANES round, the age-specific distribution of HSV-1 prevalence was derived, as well as the age-specific distribution of self-reported ever-symptomatic and clinically diagnosed genital herpes prevalence in individuals who were concurrently HSV-1 antibody positive and HSV-2 antibody negative . This distinction ensures that genital herpes cases are attributed to HSV-1, as the presence of HSV-1 antibodies and the absence of HSV-2 antibodies indicate that the infection was acquired through HSV-1 rather than HSV-2.
Additionally, the distribution of the reported number of sexual partnerships in the past 12 months was derived, along with the age-specific distribution of sexual partnerships during the same period.
Model Calibration
The model was first fitted to the population size projections for the US, as provided by the Population Division of the United Nations Department of Economic and Social Affairs . Fitting was performed using a nonlinear least-squares method, implemented with the Nelder-Mead simplex algorithm .
Subsequently, the model was fitted to NHANES time-series and age-specific data for HSV-1 prevalence and self-reported ever-symptomatic HSV-1 genital herpes prevalence using a Bayesian inference framework. The prevalence data, reported as proportions bounded between 0 and 1, were modeled using a beta distribution likelihood function.
Let P t(a) denote the model-predicted prevalence for a specific age group a at time t. The observed prevalence for the corresponding age group and time, Y t(a) , was assumed to follow a beta distribution:
Y t(a)∼Beta(α t(a),β t(a))
where the beta distribution parameters α t(a) and β t(a) were determined using the mean and variance of the distribution. The mean was set equal to the model-predicted prevalence, while the variance was derived from the 95% confidence interval of the NHANES-measured prevalence for the corresponding age group and time period.
Seven model parameters were estimated within this Bayesian framework, including ε c h i l d h o o d and ε a d u l t h o o d, as well as 5 parameters characterizing the temporal variation in oral exposure risk to HSV-1 infection within the US population, and the overall exposure risk through oral sex. Broad uniform prior distributions were assigned to all parameters to reflect minimal prior information. The priors for ε c h i l d h o o d and ε a d u l t h o o d were assumed to be Uniform(0,1) distributions covering their full possible ranges. The prior distributions for the other parameters were informed by previous fitting of these parameters .
The model was solved numerically using MATLAB R2019a to generate the model-predicted prevalence at the observed NHANES time points. Bayesian inference was performed using Markov chain Monte Carlo sampling to generate posterior distributions for the model parameters. The sampling process employed a reversible Markov chain with a stationary distribution corresponding to the target posterior distribution.
The Metropolis-Hastings algorithm was used to estimate the model parameters by iteratively proposing new parameter values from a truncated normal proposal distribution, with the mean set to the current parameter value and truncation ensuring all sampled values were valid. Proposed values were accepted or rejected based on the ratio of the posterior densities. Initial values for the parameters were randomly drawn from their respective prior distributions. Three parallel chains were run, each initialized independently, and the first half of the iterations were discarded as burn-in . The algorithm was executed for a sufficient number of iterations to ensure convergence.
Parameter estimates were calculated as the means of the posterior samples, with 95% credible intervals (95% CrIs) used to quantify uncertainty. Convergence diagnostics, including the Rhat statistic (Gelman-Rubin diagnostic), effective sample size, and autocorrelation, were evaluated to ensure proper convergence. Posterior predictive checks were performed to assess the agreement between model-predicted prevalence and observed prevalence data. Accordingly, this Bayesian calibration framework facilitated robust parameter estimation while accounting for the variability and bounded nature of the observed prevalence data.
Notably, NHANES HSV-1 surveys did not include children aged 0–4 years. Consequently, model calibration to these data cannot account for mixing patterns within this age group, limiting the model's applicability to older children.
Oversight
This study is based on mathematical modeling using publicly available data; therefore, no patient consent or ethical approval is required.
RESULTS
The model demonstrated robust fits to US population size (Supplementary Figure 1), age-specific HSV-1 prevalence data across all NHANES rounds (Figure 1), the temporal trend of HSV-1 prevalence (Figure 2A), and the temporal trend of ever-symptomatic HSV-1 genital herpes prevalence (Figure 2B).
Figure 1.
Fitting of age-specific herpes simplex virus type 1 (HSV-1) prevalence for each National Health and Nutrition Examination Survey (NHANES) round. Comparison of the model-fitted HSV-1 prevalence for each 5-year age band in the United States with NHANES data from 1976 to 2016. Abbreviations: CI, confidence interval; HSV-1, herpes simplex virus type 1; NHANES, National Health and Nutrition Examination Survey.
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Figure 2.
Fitting of herpes simplex virus type 1 (HSV-1) prevalence temporal evolution. A, Comparison of the model-fitted temporal trends in HSV-1 prevalence among individuals aged 10–49 years in the United States (US) with National Health and Nutrition Examination Survey (NHANES) data. B, Comparison of the model-fitted temporal trends in ever-symptomatic HSV-1 genital herpes prevalence among individuals aged 20–49 years in the US with NHANES data. Abbreviations: CI, confidence interval; HSV-1, herpes simplex virus type 1; NHANES, National Health and Nutrition Examination Survey.
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The modeled transmission dynamics indicate a sustained decline in both the HSV-1 oral force of infection and HSV-1 prevalence over the past few decades (Figure 2A). As a result, the age at which HSV-1 prevalence reaches 50% has steadily increased (Figure 1), shifting from the age group 20–24 years in 1990 and 2000 to 25–29 years in 2010 and 35–39 years in 2020.
Figure 3A and 3B show the model-estimated distributions for the degree of assortativeness among children aged 0–14 years and adults aged 15–99 years, respectively. The model estimated the degree of assortativeness for children (ε c h i l d h o o d) as 0.87 (95% CrI, .64–.99) and for adults (ε a d u l t h o o d) as 0.04 (95% CrI, .004–.10) (Figure 3C).
Figure 3.
Degree of assortativeness in herpes simplex virus type 1 infection transmission among children and adults. A, Model-estimated distribution of the degree of assortativeness among children aged 0–14 years. B, Model-estimated distribution of the degree of assortativeness among adults aged 15–99 years. C, Model-estimated mean and 95% credible interval (CrI) for the degree of assortativeness among children and adults.
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Supplementary Figure 2 illustrates the distributions of the 5 additional model parameters estimated in this study. These parameters include those characterizing the variation in exposure risk to oral HSV-1 infection within the US population over time: Z, ρ X(a,i)O r a l, ξ T u r n i n g, and ξ D u r a t i o n (Supplementary Figure 2A–D), as well as the overall exposure risk through oral sex: C O r a l S e x (Supplementary Figure 2E). The figure also presents the mean estimates and their corresponding 95% CrIs. Definitions and details on these parameters are available in Ayoub et al .
DISCUSSION
This study provides evidence of age-related patterns in HSV-1 transmission, revealing distinct dynamics between children and adults. Among children, specifically those older than 5 years, HSV-1 transmission exhibits strong age assortativity, with most infections acquired from peers within the same age group. This pattern suggests that age-specific interactions, such as close-contact activities and shared environments—including daycare centers, schools, and playgrounds—play a major role in sustaining HSV-1 transmission in this demographic. In contrast, for younger children, existing literature indicates that household contacts, particularly parents, are the primary source of HSV-1 transmission .
In contrast to children, HSV-1 transmission among adults is weakly assortative by age group. HSV-1 acquisitions in adults are distributed across transmissions from a wide range of age groups, with no single age group predominating as the primary source of viral transmission. This pattern suggests that adult transmission dynamics are driven by more heterogeneous interaction patterns, influenced by diverse social and behavioral factors. These factors may include varied social, occupational, and lifestyle interactions that bridge age groups and facilitate cross-age group exposure.
The observed lack of age-assortative mixing among adults in HSV-1 oral transmission contrasts with the strong age-assortative patterns seen in the sexual transmission of sexually transmitted infections [43, 44]. In the latter, men within a specific 5-year age group typically preferentially mix with women in the adjacent younger 5-year age group [43, 44].
Since viruses such as HSV-1 propagate through social networks, their transmission patterns offer insights into the underlying structures of these networks. The findings suggest that, unlike adults, children's social networks are high-density, age-dependent systems characterized by typical small-world properties . These small-world properties include high clustering, indicating tightly connected groups, and short path lengths, while still maintaining some long-range connections, which enable efficient transmission of infection while balancing local clustering with global reach. These networks may also exhibit a relatively homogeneous distribution of both interaction time and interaction partners, reflecting the structured and frequent interactions typical of children's social environments.
These findings may have implications for other infections transmitted through close-proximity interactions and propagated within social networks. The results align with evidence on influenza transmission patterns, such as in school settings, where strong assortative mixing is facilitated by the structural organization of schools into classes and grades [46–48]. These findings emphasize the role of age-specific interactions in shaping the transmission dynamics of such infections and underscore the importance of tailored public health interventions.
For children, targeted interventions focusing on specific environments such as schools or daycare centers may be most effective, while for adults, broader community-level strategies may be better suited for controlling the spread of such infections. Notably, HSV-1 vaccination, once available, could serve as the most effective public health intervention against HSV-1 infection [49, 50], as it would provide protection regardless of social context, interactions, or age.
This study has limitations. First, NHANES surveys did not include children aged 0–4 years, and only 2 surveys included children aged 5–9 years. As a result, the estimated assortativeness ε c h i l d h o o d is primarily informed by data from the age group 10–14 years, which was consistently available across all survey rounds. Consequently, ε c h i l d h o o d estimate is most representative of the age group 10–14 years and does not reflect assortativeness in mixing among younger children aged 0–4 years.
Second, a population-level model was used to examine the degree of age-assortative mixing; however, this type of model parameterizes interactions between age groups collectively and does not explicitly account for household interactions or prolonged household contacts, such as the extended duration of parent–child relationships or sibling interactions at home, which are particularly important during the first few years of life before children enter daycare or school . While an individual-based model could capture such effects, its implementation would still require detailed household-level data on interactions and HSV-1 biomarkers for proper calibration, which are currently unavailable. Notably, as HSV-1 prevalence continues to decline in the broader population [3, 8, 16], decreasing maternal and paternal HSV-1 prevalence may reduce parent-to-child transmission, potentially reinforcing age-assortative mixing patterns in HSV-1 transmission among children.
Third, the mixing matrix was parameterized using a conventional approach [8, 34–36], separating mixing into 2 distinct components: an assortative component based on age and a nonassortative component where mixing occurs without age preference. While this formulation is flexible and accommodates diverse mixing patterns, it is not exhaustive and does not capture other theoretically possible patterns, such as preferential assortative mixing between different age groups, for example, between mothers and their infants.
The goal of this analysis, however, is not to model all potential forms of mixing exhaustively—an approach that is not feasible given the available data for model calibration—but rather to identify a clear signature of variable assortativeness between children and adults. The markedly distinct assortativeness values observed for these 2 groups provide compelling evidence for differing transmission dynamics between children and adults.
Fourth, this study investigated HSV-1 transmission patterns within the US population, which may limit the generalizability of the findings to other populations. However, the observed patterns appear to stem from basic features of social networks that could be consistent across human populations, suggesting that the findings may be applicable, at least in part, to other contexts.
Fifth, the model did not explicitly stratify the population by sex . However, global analyses of HSV-1 epidemiology indicate no significant differences in exposure risk between females and males [20, 24–27], making this limitation unlikely to affect the results.
Finally, the model assumes that HSV-1 infectiousness does not vary with the presence of clinical symptoms and does not account for the potential impact of antiviral treatment during symptomatic episodes or suppressive therapy . While these are simplifications, their effect on the results is expected to be minimal, as the majority of infectious viral shedding occurs asymptomatically and HSV-1 infection is rarely treated [4–6].
This study has strengths. First, to the best of our knowledge, it is the first to investigate assortativeness in the age-dependent transmission patterns of HSV-1 infection. Second, the study utilized standardized, population-based data from NHANES spanning over 4 decades, providing reliable and representative estimates that reflect the sociodemographic diversity and modes of acquisition within the population [3, 16, 28–32]. The use of such representative, statistically precise input data minimized uncertainty in the results and estimates.
Third, a sophisticated mathematical model was employed to capture the complex dynamics of HSV-1 transmission, grounded in high-quality data on the natural history and transmission parameters of HSV-1 infection . Finally, the model demonstrated a robust fit to empirical data, with predicted trends closely aligning with observed patterns. This alignment supports the robustness of the model and the reliability of its findings.
In conclusion, this study identified distinct age-related patterns in HSV-1 transmission, characterized by strong age assortativity among children >5 years of age and weak assortativity among adults. These findings highlight the role of age-specific social networks in shaping transmission dynamics and may have implications for other infections transmitted through close-proximity interactions. These insights support the importance of targeted public health interventions, with strategies tailored to structured environments for children and broader community-level approaches for adults.
Supplementary Data
Supplementary materials are available at The Journal of Infectious Diseases online ( Supplementary materials consist of data provided by the author that are published to benefit the reader. The posted materials are not copyedited. The contents of all supplementary data are the sole responsibility of the authors. Questions or messages regarding errors should be addressed to the author.
Notes
Acknowledgments. The authors are grateful for infrastructure support provided by the Biomedical Research Program and the Biostatistics, Epidemiology, and Biomathematics Research Core at Weill Cornell Medicine–Qatar. The authors are further grateful for the administrative support of Ms Adona Canlas. ChatGPT was exclusively utilized to verify grammar and refine the English phrasing in our text. No other functionalities or applications of ChatGPT were employed beyond this specific scope. Following the use of this tool, the authors thoroughly reviewed and edited the content as necessary and take full responsibility for the accuracy and quality of the publication.
Author contributions. Conceptualization: L. J. A. Methodology and model development and parameterization: H. H., H. H. A., and L. J. A. Software and analysis: H. H. and H. H. A. Validation and investigation: H. H., H. H. A., and L. J. A. Writing—original draft: H. H. and L. J. A. Writing—review and editing: All authors. Supervision: L. J. A. and H. H. A.
Data availability. Data generated or analyzed during this study are included in the main text and Supplementary Material. The MATLAB codes used for the model can be obtained by contacting the authors.
Disclaimer. The funder had no role in the design and conduct of the study.
Financial support. This work was supported by the Qatar Research Development and Innovation Council (grant number ARG01-0524-230321). The content is solely the responsibility of the authors and does not necessarily represent the official views of the Qatar Research Development and Innovation Council.
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Author notes
Potential conflicts of interest. All authors: No reported conflicts.
All authors have submitted the ICMJE Form for Disclosure of Potential Conflicts of Interest. Conflicts that the editors consider relevant to the content of the manuscript have been disclosed.
© The Author(s) 2025. Published by Oxford University Press on behalf of Infectious Diseases Society of America.
This is an Open Access article distributed under the terms of the Creative Commons Attribution License ( which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited.
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11319 | https://www.youtube.com/watch?v=pzJanh-Ol4g | Gauss's Law Problem: Sphere and Conducting Shell
Physics Ninja
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Posted: 1 Feb 2020
Physics Ninja looks at a classic Gauss's Law problem involving a sphere and a conducting shell. The inner sphere can be a conductor or an insulator and the outer shell is assumed to be a conductor. Charge is placed on both the sphere and shell. We use Gauss's Law to find the Electric Field everywhere in space.
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Transcript:
hi everybody physics ninja here today what we're gonna do is we're going to apply Gauss's law this equation right over here which is the integral of the electric field scalar product with the area is equal to Q enclosed over epsilon zero we're going to apply Gauss's law in order to find the electric field everywhere in space and the geometry I'm considering here is the one shown in the figure so what we have here is a sphere at the center of a shell okay so the sphere the inner sphere has a radius a the outer shell has a thickness and the inner radius is B and the outer radius is C so how would you solve for the electric field everywhere in space and what we're gonna do is we're gonna consider two cases okay so case number one for this Inner Sphere I'm going to assume that it is a conductor okay and again that inner shell or sort of that Inner Sphere rather has a total charge equal to 3q the outer shell has a total net charge of negative Q okay so how would you set up Gauss's a lot of salt for the electric field everywhere and for the second case what I'm going to do is I'm gonna assume that this Inner Sphere is an insulator and the charge is uniformly distributed throughout the volume of that sphere okay so they've got two different cases if it's insulating versus conducting what is the difference how do you set up Gauss's law what makes it different all right so let's get started again if you liked the video give it a thumbs up consider subscribing to my channel and if you have any questions leave them in the comments section I'll get back to you okay so case one here is the case where we're going to assume that this inner sphere is conducting okay and my goal is to find the electric field in region one so anywhere within this sphere so the first thing you do for case one is if it's a conducting sphere okay this is a very very special word if you hear that word conducting sphere it means by definition okay that the electric field inside must be equal to zero how is that possible okay the only way that it's possible from Gauss's law that you get zero the only way that's possible is if being clothes charge of my Gaussian surface also equals to zero so what that means here is that this 3q must be spread out evenly on this spherical surface okay so that's this is what's going to happen for a conductor you can't have any charge anywhere inside because that would produce an electric field and then that means that the charges would move because there'd be a force acting on them okay so case one is kind of just the definition that the field inside a conductor must be zero so all of the charge is going to be on the outside okay now case two is a little bit more complicated so for case two what we're going to assume here is that the charge is going to be uniformly distributed throughout the entire volume here of all right we're gonna assume that it's uniformly distributed throughout the entire volume of the sphere okay so what we have to do now now you really have to apply Gauss's law for this so the first thing we're gonna do is again draw our Gaussian surface right and that's again it's going to look like a sphere yeah mine's a little bit rough looking that's okay and the sphere here has a certain radius let's call it radius little R like this all right so the question is how do you apply Gauss's law for this so since this is spherically symmetric actually the left-hand side of Gauss's law is always pretty straightforward okay so first of all to get rid of this integral the integral will simply simplify to something like this it's the electric field magnitude multiplied by the surface right and the reason that it simplifies is because again the electric field produced by any amount of charge inside the sphere is going to be pointing straight out and the area is also right if I look at the little bit of area of my sphere that's also a vector that points radially outward so what we need to do now is simply evaluate what is this total area of the sphere and in this case it's simply 4 PI R squared this is a formula for the surface of a sphere that has a radius R alright so now we write down the rest of Gauss's law it's the charging close than this green surface and divided by epsilon zero all right pretty straightforward now you have to use kind of your judgment here and try to evaluate how do we find how much charge is inside now it's not equal to three Q because three Q is the total charge so it's going to be a fraction of the total charge right if you think about how much charge is in close let's go ahead and write it down we get my marker all right so we have Q enclosed is really going to be a fraction of the total charge now what you could also do is you could define a charge density which equals to the total charge divided by the total volume and then integrate over the volume you really don't have to do that you could just say it's going to be a volume fraction of the total charge no so this is would be the total volume of this sphere which is 4 PI R cube and in this way it's a cube right because the radius of the sphere is a and now how much volume is enclosed here in this a green surface it would be again 4/3 PI R cube all right now we can simplify this expression a little bit the 4/3 cancel the pi cancel and my total charge is really 3 Q so at the end this here simplifies to R cube multiplied by 3 Q put the 3 in the front and divided by a cube ok so now I'm just gonna put everything together let me give myself a little bit of extra space here kind of shrink that down okay so now we plug everything into Gauss's law so again the left hand side was e multiplied by 4 PI R squared and the right hand side was Q enclosed which is my expression here divided by epsilon zero so it's just three our big Q and divided by epsilon zero a cube ok we could simplify a few of the terms here first of all you notice you have R squared here and you have R cube here which means you could get rid of two of them and get rid of the two up here you're still left with one and at the end you just want one final expression for my electric field magnitude so I bring the 4pi down at the bottom so you get 1 over 4 PI epsilon 0 you kind of always have that term right and then you look at all the terms that are left 3 Q was the charge so that term is there and I still have divided by a cube that's just a constant term that's the radius of this sphere and then at the end I can't forget this R and this is really really important right so this is it depends linearly with the distance away from the center so to kind of really different results right if it's insulating and the charge is uniformly distributed this is what you get and if it's a conducting sphere you would get zero okay all the way up until the surface alright so now let's consider the second region so for region - now region two is in this white area this white space between the sphere and that outer shell and again what you first do is you draw a Gaussian surface somewhere within that white region and my goal now is to write down Gauss's law so again it's spherically symmetric so the left-hand side of Gauss's law basically always reduces to this 4 pi and the area of this sphere is 4 PI R squared okay that was a left-hand side of Gauss's law equals to Q enclosed divided by my constant epsilon 0 so now you ask yourself how much charge is enclosed by this shell or by this Gaussian surface rather and again if you have a look at the diagram how much charge is enclosed well all of this charge that is inside this Inner Sphere is enclosed right and whether it's conducting or whether its insulating it really doesn't matter because that total charge was 3 Q right the only difference if it's conducting or insulating it's the way that the charge is spread out but really this charge in closed is always 3 Q so I can just go ahead and just write it down that's the total charge enclosed divided by Epsilon zero and again just rewrite the left-hand side of Gauss's law here and again bring the four PI R squared at the bottom and this is what we're left with total charge is three Q divided by four PI epsilon zero multiplied or sorry divided by R squared like this all right so this looks like a familiar expression right this looks like exactly the field produced by a point charge that would have a charge equal to three Q and that charge would all be concentrated at one point right and if I'm a distance R away this would be the expression I would use to find the magnitude of the field produced by that point charge okay it's kind of a nice result from Gauss's law all right let's consider the third region now so Region three now is anywhere inside this outer shell however in the statement of the problem I said something really really important okay I said that this outer shell is a conductor okay and this is really really the key to this problem right here so if it's a conductor you should automatically know the field inside anywhere inside this the field inside the outer shell let's just write it as e subscript shell must be equal to zero it's a conductor now if you think back of our Gauss's law well think about our Gauss's law how would we get zero right how would we get zero for the electric field in this region well let's write down Gauss's law on the left hand side of Gauss's law would be multiplied by four PI R squared again this is a spherically symmetric object so this is how it would look like and the area of my Gaussian surface over here is four PI R squared now this has to be equal to Q enclosed divided by epsilon zero but how do we get Q enclosed for this problem well let's think about how much charge is enclosed here all right so we have charged and closed we definitely have enclosed all of this right because my Gaussian surface is out here and have 3q okay but I do require this stamen right how do I get zero electric field the only way I can really have zero electric field is if my queueing clothes must also be equal to 0 if Q enclosed is zero then automatically the field is going to be zero so that means that there has to be some charge that has to go on this inner wall of the shell and now the question is how much charge goes on this inner wall well let's we have to add it up because it's going to be enclosed by this Gaussian surface so it's gonna be plus Q I'll just write it as inner wall okay so at the end of the day we do require that the Q enclosed over here is equal to zero and the only way you can have this because I do have the 3 Q enclosed from this sphere that means that the inner wall Q inner wall must be opposite of whatever the total charges from this sphere so at the end of the day I find that the only way I can have zero electric field inside this conductor is if the charge on this inner wall is equal to negative 3 Q this is a requirement and this will ensure that the total charge enclosed is going to be 0 and that is going to force that electric field to also be zero okay so let me go ahead and write this so Q inner wall must be equal to negative 3 Q all right so this way you add negative 3 Q to the plus 3 Q of the sphere and you're going to get zero total charge enclosed if I have zero total charge enclosed I'm going to get zero electric field anywhere in this region all right so the next question we have to ask ourselves is well if this inner wall has negative 3 Q like we calculated here what about the outer wall right how much charge is actually on this surface over here of that in order to answer that you simply have to look at the total charge of that conductor in this problem I said that the total charge of the conductor was negative Q all right so this is kind of oil it looks like right so Q total for the shell has to be equal to whatever is on the inner wall inner I'll just write it as Q inner plus whatever is on the outer wall okay and the total charge of the shell is given by this number negative Q all right this is what we had this was a negative Q we just solved for what was on this inner wall the inner wall we said was negative 3q so plus Q outer so at the end now you just bring the negative 3q on the other side you're left with that the charge on the outer surface charge on the outer surface must be equal to 2q you have no choice you have to have conservation of charge so if I put negative Q on here that means that on the inner wall I'm gonna get negative 3q and on the outer wall I have to have plus 2 Q that's the only way that both of those are going to sum up to equal to the total charge on the shell okay because negative 3 plus 2 gives me negative 1 which is what I said in the problem statement and you have this distribution of charge because we do require that the field is equal to 0 everywhere in this shell because it's a conductor all right let's go on to a little final region okay so this is now region 4 what I've drawn is a Gaussian surface that is on the outside because this is where I want to evaluate the field I want to evaluate it when the radius is bigger than C so I want to be on the outside of that conducting shell all right again we apply Gauss's a lot of this problem we want to look at the field dotted with the area it's a spherical surface so the area of that sphere is 4 PI R squared always the same thing for spherically symmetric objects all right this must be equal to again how much charge is enclosed by that surface divided by epsilon zero well now let's look at what is Q and closed for this problem well number one I am enclosing this entire sphere right I definitely have all of that charge so if you go ahead and write this you have to have definitely plus 3 q is enclosed by this Gaussian surface what else I am also enclosing all of the charge that is on the shell and all of the charge on the shell is well it's negative Q so at the end what I have is 2 Q this has to be the total charge enclosed by my Gaussian surface in this case so we go ahead and we substitute that into Gauss's law so you get e 4 PI R squared must be equal to 2 Q divided by epsilon 0 to get the final expression you just bring all of this term in the bracket here down in the denominator on the other side so you'll get 2 Q divided by 4 PI epsilon 0 and over R squared again if you look at this result this would be the result that you would get if you had a point charge and if the point charge was equal to 2 Q and I was a certain distance R away from that point charge right this is if I'm evaluating what is the field at this point I would get the exact same result okay and that's kind of obtained from Gauss's law this way okay so here's a summary of the results that we obtained let's try to make a sketch now so for the region from what I'm plotting here is the magnitude of the electric field it just right is e here on the y axis and I have the distance R on this x axis and again let's draw the different cases so the first one we're gonna do is well if it's a conducting sphere then you should have zero here now this other one is if it's insulating let me put in a different color over here it should be a linear relationship and it should go all the way to the top over here okay so the field grows as I get away from the distance because I end up enclosing more charge alright and let's do the second region the field is kind of the same it starts off in both cases up here and it rolls off as one over R squared so it should look you know something like this over here all right should roll off here and this is like a 1 over R squared dependence right and what about the next part this is the region here in the shell between B and C so in that case that case is pretty easy to draw it should just be 0 cuz it's a conductor and in the last region again it should probably start at some value over here it's gonna be slower than this because I'm further out and again it's gonna roll off as one over R squared again this is proportional to the distance squared all right this is kind of what it looks like again in these regions here you could have 0 because it's a conductor and again it depends on the case here that I looked at but this is what a sketch would look like for this electric field alright thanks for watching folks hopefully you understood it and you become a better problem solver |
11320 | https://redanhs.dekalb.k12.ga.us/Downloads/CCGPS%20Unit%203%20Linear%20and%20Exponential%20Functions.pdf | CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 1 of 30 Linear and Exponential Functions Name: __ Date: ___ Represent and solve equations and inequalities graphically MCC912.A.REI.10 Understand that the graph of an equation in two variables is the set of all its solutions plotted in the coordinate plane, often forming a curve (which could be a line). (Focus on linear and exponential equations and be able to adapt and apply that learning to other types of equations in future courses.) MCC9‐12.A.REI.11 Explain why the x‐coordinates of the points where the graphs of the equations y = f(x) and y = g(x) intersect are the solutions of the equation f(x) = g(x); find the solutions approximately, e.g., using technology to graph the functions, make tables of values, or find successive approximations. Include cases where f(x) and/or g(x) are linear, polynomial, rational, absolute value, exponential, and logarithmic functions. Understand the concept of a function and use function notation MCC9‐12.F.IF.1 Understand that a function from one set (called the domain) to another set (called the range) assigns to each element of the domain exactly one element of the range. If f is a function and x is an element of its domain, then f(x) denotes the output of f corresponding to the input x. The graph of f is the graph of the equation y = f(x). (Draw examples from linear and exponential functions.) MCC9‐12.F.IF.2 Use function notation, evaluate functions for inputs in their domains, and interpret statements that use function notation in terms of a context. (Draw examples from linear and exponential functions.) MCC9‐12.F.IF.3 Recognize that sequences are functions, sometimes defined recursively, whose domain is a subset of the integers. (Draw connection to F.BF.2, which requires students to write arithmetic and geometric sequences.) Interpret functions that arise in applications in terms of the context MCC9‐12.F.IF.4 For a function that models a relationship between two quantities, interpret key features of graphs and tables in terms of the quantities, and sketch graphs showing key features given a verbal description of the relationship. Key features include: intercepts; intervals where the function is increasing, decreasing, positive, or negative; relative maximums and minimums; symmetries; end behavior; and periodicity. (Focus on linear and exponential functions.) MCC9‐12.F.IF.5 Relate the domain of a function to its graph and, where applicable, to the quantitative relationship it describes. (Focus on linear and exponential functions.) MCC9‐12.F.IF.6 Calculate and interpret the average rate of change of a function (presented symbolically or as a table) over a specified interval. Estimate the rate of change from a graph. (Focus on linear functions and intervals for exponential functions whose domain is a subset of the integers.) Analyze functions using different representations MCC9‐12.F.IF.7 Graph functions expressed symbolically and show key features of the graph, by hand in simple cases and using technology for more complicated cases. (Focus on linear and exponential functions. Include comparisons of two functions presented algebraically.) MCC9‐12.F.IF.7a Graph linear and quadratic functions and show intercepts, maxima, and minima. MCC9‐12.F.IF.7e Graph exponential and logarithmic functions, showing intercepts and end behavior, and trigonometric functions, showing period, midline, and amplitude. MCC9‐12.F.IF.9 Compare properties of two functions each represented in a different way (algebraically, graphically, numerically in tables, or by verbal descriptions). (Focus on linear and exponential functions. Include comparisons of two functions presented algebraically.) Build a function that models a relationship between two quantities MCC9‐12.F.BF.1 Write a function that describes a relationship between two quantities. ★ (Limit to linear and exponential functions.) MCC9‐12.F.BF.1a Determine an explicit expression, a recursive process, or steps for calculation from a context. (Limit to linear and exponential functions.) MCC9‐12.F.BF.1b Combine standard function types using arithmetic operations. (Limit to linear and exponential functions.) MCC9‐12.F.BF.2 Write arithmetic and geometric sequences both recursively and with an explicit formula, use them to model situations, and translate between the two forms. Build new functions from existing functions MCC9‐12.F.BF.3 Identify the effect on the graph of replacing f(x) by f(x) + k, k f(x), f(kx), and f(x + k) for specific values of k (both positive and negative); find the value of k given the graphs. Experiment with cases and illustrate an explanation of the effects on the graph using technology. Include recognizing even and odd functions from their graphs and algebraic expressions for them. (Focus on vertical translations of graphs of linear and exponential functions. Relate the vertical translation of a linear function to its y‐intercept.) Construct and compare linear, quadratic, and exponential models and solve problems MCC9‐12.F.LE.1 Distinguish between situations that can be modeled with linear functions and with exponential functions. MCC9‐12.F.LE.1a Prove that linear functions grow by equal differences over equal intervals and that exponential functions grow by equal factors over equal intervals. MCC9‐12.F.LE.1b Recognize situations in which one quantity changes at a constant rate per unit interval relative to another. MCC9‐12.F.LE.1c Recognize situations in which a quantity grows or decays by a constant percent rate per unit interval relative to another. MCC9‐12.F.LE.2 Construct linear and exponential functions, including arithmetic and geometric sequences, given a graph, a description of a relationship, or two input‐output pairs (include reading these from a table). MCC9‐12.F.LE.3 Observe using graphs and tables that a quantity increasing exponentially eventually exceeds a quantity increasing linearly, quadratically, or (more generally) as a polynomial function. Interpret expressions for functions in terms of the situation they model MCC9‐12.F.LE.5 Interpret the parameters in a linear or exponential function in terms of a context. ★ (Limit exponential functions to those of the form f(x) = bx + k.) CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 2 of 30 LESSON 3.0 ALGEBRA EXERCISES Plot the equation 1. 2 3 y x 2. 1 6 3 y x 3. 2 3 3 y x 4. 2 3 6 x y 5. 5 4 x y 6. 3 y What is the solution for x and y: 7. 8. 9. X=_ Y=_ X= Y=_ X= Y=____ CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 3 of 30 Solve for x and y 9. 3 1 5 y x y x 10. 5 y x y Plot both graphs and determine the solution for x and y. Use a graphing calculator. 11. 3 1 2x y x y 12. 3x y x y 13. 1 2 2x y x y 14. 2 x y x y CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 4 of 30 Lesson 3.1 Represent Functions as Rules and Tables Vocabulary A function consists of: A set called the domain containing numbers called inputs and a set called the range containing numbers called outputs. The input is called the independent variable. The output is called the dependent variable. The output (dependent variable) is dependent on the value of the input variable. Example: Identify the domain and range of a function The input-output table represents the price of various lobsters at a fish market. Identify the domain and range of the function. Solution: The domain is the set of inputs: 1.4, 2.2, 3.2, 4.3, 5.1, 5.3. The range is the set of outputs: 7.60, 10.90, 16.10, 20.50, 25.70, 26.90. Input (pounds) 1.4 2.2 3.2 4.3 5.1 5.3 Output (dollars) $7.60 $10.90 $16.10 $20.50 $25.70 $26.90 PROBLEMS Identify the domain and range of the function. 1. 2. 3. Input 1 3 5 7 Output 0 2 4 6 Input 0 2 6 9 Output 0 1 3 5 Input 5 7 15 17 Output 3 2 1 8 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 5 of 30 Example 2 Make a table for a function The domain of the function y = x + 2 is 0, 2, 5, 6. Make a table for the function then identify the range of the function. The range of the function is 2, 4, 7, 8. x 0 2 5 6 y=x+2 0+2=2 2+2=4 5+2=7 6+2=8 PROBLEMS Make a table for the function. Identify the range of the function. 1. y = 2x -1 Domain = 0, 1, 3, 5 The range of the function is: 2. y = -4x + 3 Domain = -2, 2, 4, 5 The range of the function is: 3. y = 0.5x – 3 Domain = 0, 1, 2, 3 The range of the function is: 4. y = ½ x – 2 Domain = 2, 4, 8, 10 The range of the function is: x y=2x-1 x y=-4x+3 x y=0.5x-3 x y=½ x – 2 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 6 of 30 Example 3 Write a rule for the function Solution Let x be the input and y be the output. Realize that the output is 3 times the input. Therefore, a rule for the function is y = 3x. Input 2 4 6 8 Output 6 12 18 24 PROBLEMS Write a rule for the function 1. 2. 3. 4. Input 3 6 7 8 Output 15 30 35 40 Input 2 4 6 8 Output 3 5 7 9 Input 1 2 3 4 Output 6 5 4 3 Input 1 2 3 4 Output 4 5 6 7 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 7 of 30 Lesson 3.2 Represent Functions as Graphs Example 1 Graph a function Graph the function y=2x with domain 0, 1, 2, 3, and 4. Solution Step 1: Make an input-output table. Step 2: Plot a point for each ordered pair (x,y). X 0 1 2 3 4 y 0 2 4 6 8 PROBLEMS Graph the function 1. 3 y x Domain: 0, 1, 2, 3 2. 1 2 y x Domain: 0, 2, 4, 6 3. 2 2 x y Domain: 0, 1, 2, 3 X 0 1 2 3 y X 0 2 4 6 y X 0 1 2 3 y CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 8 of 30 Lesson 3.3 Graph Using Intercepts Vocabulary The x-coordinate of a point where the graph crosses the x-axis is the x-intercept. The y-coordinate of a point where the graph crosses the y-axis is the y-intercept. Example 1 Find the intercepts of a graph of an equation. Find the x-intercept and the y-intercept of the graph 4x – 8y = 24 Solution: To find the x intercept, replace y with a 0 and solve for x 4x – 8(0) = 24 Solve for x = 6 To find the y intercept, replace x with a 0 and solve for y 4(0) – 8y = 24 Solve for y = -3 Therefore, the x-intercept is 6. The y-intercept is -3. PROBLEMS Find the x-intercept and the y-intercept of the graph 1. 5 7 35 x y 2. 3 2 6 x y 3. 1 5 4 y x CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 9 of 30 Example 2 Use a graph to find the intercepts Identify the x-intercept and the y-intercept of the graph Solution: To find the x-intercept, identify the point where the line crosses the x-axis. The x-intercept is -3. To find the y-intercept, identify the point where the line crosses the y-axis. The y-intercept is -4. PROBLEMS: Identify the x-intercept and the y-intercept of the graph 1. 2. 3. 4. 5. 6.
CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 10 of 30 Example 3 Use intercepts to graph an equation Graph 2x + 3y = 6. Label the points where the line crosses the axes. Solution: Step 1: Find the intercepts: To find the y-intercept, set x = 0 and solve for y. 2(0) + 3y = 6 Solve for y = 2 To find the x-intercept, set y = 0 and solve for x. 2x + 3(0) = 6 Solve for x =3 Step 2: Plot the points (intercepts) on the corresponding axes. Step 3: Connect the points by drawing a line through them. 1. Graph -3x + 2y = 6. Label the points where the line crosses the axes. 2. Graph 5x - 4y = 20. Label the points where the line crosses the axes. CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 11 of 30 Lesson 3.4 Find the Slope and Rate of Change Vocabulary The slope of a line is the ratio of the vertical change (rise) to the horizontal change (run) between any two points of the line. SLOPE = RISE/RUN PROBLEMS: Find the slope of the line shown. SLOPE = RISE/RUN 1. 2. 3. Example 1 Find a positive slope Find the slope of the line shown. Solution Pick two convenient points on the line (that fall on a lattice point). Count the boxes (units) you move up. Count the boxes (units) you move to the right. Divide the number of boxes (units) you moved up by the number of boxes (units) you moved to the right to get the slope. Pick the points (1,2) and (-3,-5). You start at the lower point and move 7 boxes (units) up. Then you move 4 Boxes (units) to the right. The slope is 7 4 . CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 12 of 30 PROBLEMS: Find the slope of the line shown. 1. 2. 3. Example 2 Find a negative slope Find the slope of the line shown. Solution Pick two convenient points on the line (that fall on a lattice point). Count the boxes (units) you move up. Count the boxes (units) you move to the left. Divide the number of boxes (units) you moved up by the number of boxes (units) you moved to the left to get the slope. Pick the points (1,3) and (-2,4). You start at the lower point and move 1 box (units) up. Then you move 3 Boxes (units) to the left. The slope is 1 3 . CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 13 of 30 Lesson 3.5 Graph Using Slope-Intercept Vocabulary A linear equation (straight line relating x and y) of the form y = mx + b is written in slope-intercept form. The letter m stands for the slope (how steep the line is) and the letter b for the y-intercept (where the line crosses the y-axis). Two parallel lines will not intersect each other and have the same slope. Two lines are perpendicular to each other if they intersect each other at 90˚. Their slopes are negative reciprocals. For example if a line has a slope of 4 than a line perpendicular to that line will have a slope of -¼ (which is the negative reciprocal of 4). Example 1 Identify the slope and the y-intercept a. 1 5 4 y x Solution: The equation is in the form y = mx + b. The slope is ¼. The y-intercept is 5. b. 5 6 12 x y Solution: The equation is not in the form y = mx + b. Rewrite the equation in slope-intercept form by solving for y. 5 6 12 6 5 12 5 5 2 6 6 x y y x Add xtoeachside y x Divideeachsideby The slope is 5/6. The y-intercept is 2. PROBLEMS: Find the slope and y-intercept of the line shown. 1. y = 5x – 6 2. y = ½ x +3 3. y = -6x + 4 4. y = -8x 5. 2x + 3y = 6 6. y = 7 + 3x CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 14 of 30 Example 2: Graph the equation 2x + y = 3 using slope intercept form. Solution: Step 1: Rewrite the equation in slope-intercept form: y= -2x + 3 Step 2: Identify the slope and the y-intercept: slope: -2 y-intercept: 3 Step 3: Mark the point (0,3) as y-intercept on the y-axis. Step 4: From the y-intercept draw a slope of -2. -2 can be rewritten as 2 2 1 . Therefore, you rise 2 and run -1. That means from the y-intercept of 3 you go up 2 (in the positive y-direction) and then 1 to the left (in the negative x-direction). y x PROBLEMS: Graph an equation using slope intercept form 1. y = 5x – 6 2. y = ½ x +3 3. 2y + 6x = 4 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 15 of 30 Lesson 3.6 Predict with Linear Models Vocabulary A line that best represents a trend in data or points is called the best-fitting line. Using a line or its equation to approximate values between two known points is called linear interpolation. Using a line or its equation to approximate values outside the range of two known points is called linear extrapolation. Example 1 Find the equation of the best fitting line. You are given following data: X -1 0 1 2 3 4 y 7 1 -2 -3 -7 -10 Find the equation of the best-fitting line for the data. Solution: Step 1: Draw a straight line representing the points. Step 2: Find the equation of the line. The y-intercept is 2 and the slope is -3. Therefore, the equation of the line is y = -3x + 2 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 16 of 30 PROBLEMS: Find the equation of the best fitting line. 1. 2. 3. 4. Make a scatter plot of the data. Then find the equation of the best fitting line. x -3 -2 0 1 3 4 y -8 -4 -2 0 2 6 5. Make a scatter plot of the data. Then find the equation of the best fitting line. x -3 -2 0 2 3 4 y 3 2 -1 0 -1 -2 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 17 of 30 Lesson 3.7 Comparing Linear and Exponential Functions Vocabulary A linear function can be represented in a straight line in the form of .
y mx b A exponential function can be represented in a curved line and has the form (1 ) .
x y a b Example 1 John deposits $300 into an account which earns 8% interest each year on the original deposit. Jane deposits $300 into an account which earns 8% interest each year on the year’s end balance. How much money is in each account after 3 years? Solution Firstly, 2% has to be converted to a decimal: 8 8% 0.08 100 John’s interest for each year is: $300 0.08 $24 Therefore, the table below shows the balance of John’s account after each of the 3 years: Jane’s interest for year 1 is just the same as John’s: $300 0.08 $24. Therefore, Jane will have a balance of $324 on her account. However, for year 2, the interest is computed using the balance of $324: $324 0.08 $26. The interest of $26 is added to the balance of $324 to yield an account balance of $350 (324+26=350). Therefore, for year 3, the interest is computed using the balance of $350 is: $350 0.08 $28. Adding the interest of $28 to the account balance of $350 yields $378. The table below shows the balance of Jane’s account after each of the 3 years: While John gets an identical interest payment of $24 per year Jane’s interest payment increases each year since she earns interest on the interest accumulated. John’s interest can be explained as a linear function (same interest payment each year) while Jane’s interest can be modeled with an exponential function (interest payment increases each year). Jack’s Account Balance Year 1 Year 2 Year 3 $324 $348 $372 Jane’s Account Balance Year 1 Year 2 Year 3 $324 $350 $378 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 18 of 30 PROBLEMS 1. Abdul deposits $500 into an account which earns 12% interest each year on the original deposit. Max deposits $500 into an account which earns 12% interest each year on the year’s end balance. How much money is in each account after 3 years? Show your answer in table format. 2. Ted deposits $10,000 into an account which earns 9% interest each year on the original deposit. Rick deposits $10,000 into an account which earns 9% interest each year on the year’s end balance. How much money is in each account after 3 years? Show your answer in table format. 3. Plot the table for Abdul and Max: Years on the x-axis and interest earned (account balance – initial deposit) on the y-axis. Abdul Max Which one has a straight line and which one shows an upward curved line? Which one is linear and which one is exponential? Abdul’s Account Balance Year 1 Year 2 Year 3 Max’ Account Balance Year 1 Year 2 Year 3 Ted’s Account Balance Year 1 Year 2 Year 3 Rick’s Account Balance Year 1 Year 2 Year 3 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 19 of 30 4. To encourage communication between parents and their children and to prevent children from having extremely large monthly bills due to additional minute charges, two cell phone companies are offering special service plans for students. Talk Fast cellular phone service charges $0.10 for each minute the phone is used. Talk Easy cellular phone service charges a basic monthly fee of $18 plus $0.04 for each minute the phone is used. Your parents are willing to purchase for you one of the cellular phone service plans listed above. However, to help you become fiscally responsible they ask you to use the following questions to analyze the plans before choosing one. a. How much would each company charge per month if you talked on the phone for 100 minutes in a month? How much if you talked for 200 minutes in a month? b. Build a table and make a graph for Talk Fast: X (number of minutes) Y (cost in $) c. Write a function rule (in the form y=mx+b), where y represents the cost ($) and x represents the minutes. CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 20 of 30 d. Build a table and make a graph for Talk Easy: X (number of minutes) Y (cost in $) e. Write a function rule (in the form y= mx+b), where y represents the cost ($) and x represents the minutes. f. Which company would be a better financial deal if you plan to use the phone for 200 minutes a month? Explain your reasoning. g. Which company would be a better financial deal if you plan to use the phone for 500 minutes a month? Explain your reasoning. CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 21 of 30 5. Compare the graphs below. a. Which one is shown as a straight line and which one is curved? ( ) (1 0.5)x f x 1 ( ) 3 2 g x x b. Show the graphs in table format. 3 2 1 0 1 2 3 4 5 1 ( ) 3 2 g x x ( ) (1 0.5)x f x c. As the values of x increase by 1 what happens to the corresponding y-values of ( )?
g x d. As the values of x increase by 1 what happens to the corresponding y-values of ( )?
f x e. Which function increases in same increments? That function is called linear function. f. Which function increases in “growing” increments? That function is called exponential function. g. Write down an equation for a linear function (different from above) and plot the function. h. Write down an equation for an exponential function (different from above) and plot the function. CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 22 of 30 Lesson 3.8 Explicit and Recursive Formulas Vocabulary An explicit formula allows direct computation of any term for a sequence 1 2 3 4 , , , ,...
,....
n a a a a a 1 ( 1) n a a n d where 1 a is the first term, and d is the difference between subsequent terms. Example: 1 2 3 4 2, 5, 8, 11,......
a a a a Therefore, 1 2 a , and 3.
d To find any term in the sequence plug the values for 1 a and d into the formula: 1 ( 1) 2 ( 1) 3 n n a a n d a n For a sequence 1 2 3 4 , , , ,...
,....
n a a a a a a recursive formula is a formula that requires the computation of all previous terms in order to find the value of .
n a Example: 1 1 3 2 5 n n a a a 1 2 1 2 1 1 3 1 3 1 2 4 1 4 1 3 3 2 5 2 5 2 5 2(3) 5 11 2 5 2 5 2 5 2(11) 5 27 2 5 2 5 2 5 2(27) 5 59 .
n n n a a a a a a a a a a a a a etc Example 1 Write the terms of a sequence. Write the first five terms of a. 4 3 n a n b. 1 ( 1)n n a Solution: Because no domain is specified, start with n=1. a. b. 1 2 3 4 5 4(1) 3 7 4(2) 3 11 4(3) 3 15 4(4) 3 19 4(5) 3 23 a a a a a 1 1 1 2 1 2 3 1 3 4 1 4 5 1 5 ( 1) 1 ( 1) 1 ( 1) 1 ( 1) 1 ( 1) 1 a a a a a CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 23 of 30 PROBLEMS Write the first six terms of the sequence. 1. 3 n a n 2. 4 5 n a n 3. 1 2n n a 4. ( 1) 2 n n a n PROBLEMS Describe the pattern, write the next 3 terms, and state a rule for the nth term of the sequence. 5. 3,6,9,12,... 6. 5, 4, 3, 2,... Example 2 Describe the pattern, write the next 3 terms, and state a rule for the nth term of the sequence 2, 6 12, 20, … Solution: The difference between 2 and 6 is 4, the difference between 6 and 12 is 6, and the difference between 12 and 20 is 8. Therefore, the next difference is likely to be 10, then 12 , then 14, etc. Accordingly the next three numbers in the sequence should be 30, 42, and 56. To state a rule in mathematical terms you have to realize that the terms 2, 6, 12, 20 can be written as 1(2), 2(3), 3(4), 4(5). The next term should be 5(6) which is 30. Therefore a rule for the nth term is ( 1).
n a n n CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 24 of 30 7. 1 1 1 1 , , , ,...
1 3 5 7 8. 2 3 4 5 , , , ,...
3 4 5 6 CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 25 of 30 Lesson 3.9 Arithmetic Sequences and Series Goal: Study arithmetic sequences and series. In an arithmetic sequence, the difference of consecutive terms is constant. That means the difference between any two consecutive terms remains the same. This difference is called common difference and is denoted by d in the formula below. The nth term of an arithmetic sequence with first term 1 a and common difference d is given by: 1 ( 1) n a a n d The expression to add the terms in an arithmetic sequence is called an arithmetic series. The sum of n terms is given by: 1 2 n n a a S n PROBLEMS Identify arithmetic sequences. Which ones of the following sequences are arithmetic? 1. 3,6,9,12,..... 2. 4,8,12,16,.. 3. 8,6,4,2, 2,... 4. 1,3,5,7,11,13,... Example 1 Identify arithmetic sequences. Which ones of the following sequences is arithmetic? a. 2,4,6,8,..... Solution: Yes, because the difference between all terms is 2. b. 1,4,7,9,..... Solution: No, because the difference between all terms is not the same. c. 5,9,13,17,..... Solution: Yes, because the difference between all terms is 4. CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 26 of 30 PROBLEMS Write a rule for the nth term of the sequence. Then find 15.
a 5. 5,7,9,11,13,... 6. 6,11,16,21,... 7. 4,3,2,1,... 8. 4,2,8,14,20,... 9. 25, 29, 33, 37,... Example 2 Write a rule for the nth term of the sequence. Then find 15.
a 19,23,27,31,35,... Solution: The difference between each term is 4.Therefore 4.
d The first term is 19.Therefore, 1 19.
a Plug the values into the formula 1 ( 1) 19 ( 1) 4.
n a a n d n Therefore, the rule for the nth term is: 19 ( 1) 4.
n a n To find the 15th term or 15 a replace n with 15: 15 19 (15 1) 4 19 14 4 75.
a CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 27 of 30 PROBLEMS Find the sum of the first n terms of the arithmetic series. 10. 5,7,9,11,13,...; 19 n 11. 25,35,45,55,...; 50 n 12. 4,3,2,1,...; 30 n 13. 5,8,11,14,...; 10 n Example 3 Find the sum of the first 25 terms of the arithmetic series19,23,27,31,35,.... Solution: The difference between each term is 4.Therefore 4.
d The first term is 19.Therefore, 1 19.
a Plug the values into the formula 1 ( 1) 19 ( 1) 4.
n a a n d n Therefore, the rule for the nth term is: 19 ( 1) 4.
n a n To find the 25th term or 25 a replace n with 25: 25 19 (25 1) 4 19 24 4 115.
a Plug the values for 1 25 , , a a d into the formula 1 2 n n a a S n or = 25 19 115 25 1675 2 S CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 28 of 30 Example: Find an explicit and recursive formula for the sequence 5,8,11,14,17,.... Solution: An explicit formula can be written in the form 1 ( 1) n a a n d where 1 a is the first term, and d is the difference between subsequent terms. The first term, 1 5 a . The difference between each term, 3.
d To find any term in the sequence plug the values for 1 a and d into the formula: 1 ( 1) 5 ( 1) 3 n n a a n d a n To check whether the explicit formula for the sequence is correct check by putting in the values for 1 a and d for let’s say the 4th term: 4 1 ( 1) 5 (4 1)3 5 (3)3 14 a a n d This is indeed correct. A recursive formula is a formula that requires the computation of all previous terms in order to find the value of .
n a In our case 1 5 a . The next term can be written as 1 3.
n n a a To check whether this is correct put in the values for the first 4 terms: 1 2 1 2 1 1 3 1 3 1 2 4 1 4 1 3 5 3 3 3 5 3 8 3 3 3 8 3 11 3 3 3 11 3 14 .
n n n a a a a a a a a a a a a a etc CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 29 of 30 SEQUENCES ARE FUNCTIONS 14. Represent the function ( ) 2 1 f n n in table form and graphically. Fill in the remaining points. 0 1 2 3 4 5 ( ) 2 1 f n n 1 3 10 10 15. Write an explicit formula for the function in the form 1 ( 1) n a a n d where 1 a is the first term and d is the difference between two consecutive terms. 16. Write a recursive formula for the function. (Example : 1 1 3 5 n n a a a . The next term is expressed in terms of the previous term). CCGPS UNIT 3 – Semester 1 COORDINATE ALGEBRA Page 30 of 30 17. Represent the function ( ) 3 f n n in table form and graphically. 0 1 2 3 4 5 ( ) 3 f n n 10 10 18. Write an explicit formula for the function in the form 1 ( 1) n a a n d where 1 a is the first term and d is the difference between two consecutive terms. 19. Write a recursive formula for the function. (Example : 1 1 3 5 n n a a a The next term is expressed in terms of the previous term). |
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What is Bass and Treble?
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Can someone please explain the difference of bass and treble as if to someone with no background knowledge in music? Every time I ask I someone, they always answer as if I'm already an expert on music. They use terms like "the thinness or thickness of a mix", "low end and high end frequencies", "air", "depth", "tinny" and many other terminology I don't understand. And if I hear an audio demonstration I don't know what I'm supposed to listening for and it all sounds the same to me.
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edited Aug 12, 2018 at 17:08
Dom♦
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asked Aug 5, 2018 at 16:41
AlanAlan
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Do you understand what a "low sound" is and a "high sound"?
Draakhond
– Draakhond
2018-08-06 10:40:00 +00:00
Commented Aug 6, 2018 at 10:40
I assume one is low pitched and the other is high pitched. However I see people describing two sounds that sound the same as being both
Alan
– Alan
2018-08-06 11:11:03 +00:00
Commented Aug 6, 2018 at 11:11
I'm voting to close this question as off-topic because questions about music practice, theory, terminology, etc. are off-topic.
user7708
– user7708
2019-11-16 01:12:31 +00:00
Commented Nov 16, 2019 at 1:12
2
@Maika_Sakuran0miya, Bass and Treble are settings that can be find with music listening devices, hence can be associated with music enjoyment. You need to know what these settings mean if you want to know how to properly adjust your audio listening device.
Bebs
– Bebs
2019-11-25 08:26:27 +00:00
Commented Nov 25, 2019 at 8:26
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Sound is created by vibrations. How fast those vibrations are is called "frequency." There is a range of vibrations that the human ear is sensitive to. The slower, bigger vibrations in this range are called "bass." The faster, smaller vibrations are called "treble." Everything else is called "midrange." Many sounds can be a mixture of both kinds of vibrations, and (to add to the confusion) bass notes can generate a kind of "ghost tone" over top of them in the treble range, called "overtones".
Usually bass sounds are conceptualized spatially as "low," and treble sounds as "high." This can cause confusion with (for example) a guitar, where the (larger, thicker) bass strings are at the top, and the treble strings at the bottom. A good way to think of bass versus treble is that bass is characteristic of the voice of (some) adult males, with treble being more like the typical voice of a little girl.
In an audio system, bass sounds are created by large speakers called woofers and sub-woofers, and can vibrate your entire body if they are loud enough. Treble sounds are created by tiny speakers called tweeters, and can be very ear-piercing. Another difference is that treble sounds are experienced as coming from a specific direction, while bass is largely non-directional (because it washes over your whole body). If you have earphones, and you hold them at a distance from your ear, you will only hear the treble. If you press them into your ear, it will tend to make the bass sound louder.
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edited Aug 6, 2018 at 20:43
answered Aug 6, 2018 at 20:38
Chris SunamiChris Sunami
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If you stand before a piano/keyboard, the left half is called bass, the right hand treble, therefore the corresponding clefs are called bass clef and treble clef.
Singers have more categories like soprano, alto, tenor, and bass, abbreviated to the starting letters SATB for choral works. In this context the category relates to the standard range for that voice. For instruments the specification is even more detailed and often involves their lowest note.
Older music had "alto" and "tenor" clefs : tenor clef is still used for some instruments, for example bassoon, cello, double bass, trombone and euphonium, and alto clef for the viola.
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edited Nov 2, 2019 at 12:58
Angst
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Bass is low sounds which make a kind of "Boosh" sound
Treble is high sounds which make a more "Bish" sound
Bass deep voice "oo"
Treble higher voice "i"
Take the genre trance for example
What sounds like glass bottles clanging together mixed with a sharpish clang and a "iiiiiiiii" sound is the treble
What sounds like the quiter yet heavier "oo" echo that you cant hear as much is the bass
Search DJ hero 2 tiesto i will be here and listen to about the first 20 seconds of a staticy glass sound which is the "treble" and youll notice a lesser sound behind it thats harder to hear and thats the "bass"
Treble is higher
Bass is lower
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answered Nov 6, 2019 at 9:55
Certain Trance example onlyCertain Trance example only
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Bass = power / Treble = definition, clarity, presence, if that helps any ;)
Just for reminder, it takes years of practice to master music production. Don't blame the others if they provide you "too complex" notions. Just educate yourself, be a nerd, read/watch tutorials, find people/courses which can boost your experience, pratice and be patient.
Check attackmagazine.com & adsrsounds.com, they have solid tutorials, wish you the best.
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answered Aug 5, 2018 at 18:27
CorrinoCorrino
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I've been trying to educate myself. I looked up what thinness was and it said "the lack of thickness in a mix" and when I looked up thickness it said "the lack of thinness in a mix" and most definitions were just circular and confusing
Alan
– Alan
2018-08-05 21:04:07 +00:00
Commented Aug 5, 2018 at 21:04
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AP®︎/College Calculus AB
Course: AP®︎/College Calculus AB>Unit 5
Lesson 4: Using the first derivative test to find relative (local) extrema
Introduction to minimum and maximum points
Finding relative extrema (first derivative test)
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Using the first derivative test to find relative (local) extrema
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Relative minima & maxima
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Let g(x)=x 6−3 x 5.
For what value of x does g have a relative minimum ?
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11323 | https://www.ck12.org/flexi/chemistry/wavelength-and-frequency-calculations/frequency-may-also-be-shown-as-an-si-unit-called-a-b-which-is-shown-as-1-by-s-or-s-1/ | Flexi answers - Frequency may also be shown as an SI unit called a ____ which is shown as 1/s or s-1. | CK-12 Foundation
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Frequency may also be shown as an SI unit called a ____ which is shown as 1/s or s-1.
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Frequency is measured in a SI unit called a "hertz" (Hz), which is equivalent to 1/s or s^-1. This is because frequency refers to the number of cycles per second.
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Visible light has a wavelength of 380nm-700nm. If the frequency of light is known to be 5.36 x 10^13 Hz, is the light visible? HINT: Calculate the wavelength in nm. C = 3.0 x 10^17 nm/sec, C = λf. Responses: 5600 nm, yes, it is visible, 5600 nm, no it is not visible, 0.00018 nm, yes, it is visible, 0.00018 nm, no it is not visible.How do you calculate wavelength from frequency?The UV spectrum of benzonitrile shows a secondary absorption band at 271 nm. If a solution of benzonitrile in water with concentration 1 x 10^-4 molar is examined at 271 nm, what will be the absorbance reading (ε=1000) and what will be the intensity ratio, I₀/I respectively? The cell length is 1 cm.
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11326 | https://radiopaedia.org/articles/multiple-myeloma-1?lang=us | Multiple myeloma
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Citation, DOI, disclosures and article data
Yap K, Moore C, Sharma R, et al. Multiple myeloma. Reference article, Radiopaedia.org (Accessed on 28 Sep 2025)
rID:
9555
Article created:
29 Apr 2010,
Ki Yap
At the time the article was created Ki Yap had no recorded disclosures.
View Ki Yap's current disclosures
Last revised:
14 Jun 2025,
Ashesh Ishwarlal Ranchod
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At the time the article was last revised Ashesh Ishwarlal Ranchod had
no financial relationships to ineligible companies to disclose.
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89 times, by
43 contributors -
see full revision history and disclosures
Systems:
Musculoskeletal, Haematology, Oncology
Tags:
neuroradiology, oncology, rg_39_4_edit
Synonyms:
Myelomatosis
Plasma cell myeloma
Disseminated multiple myeloma
Kahler disease
Kahler's disease
Multiple myelomas
MM (multiple myeloma)
Multiple myeloma (MM), also known by the names plasma cell myeloma and Kahler disease, is a multifocal proliferation of plasma cells based in the bone marrow. It is the most common primary malignant bone neoplasm in adults. It arises from red marrow due to the monoclonal proliferation of plasma cells and manifests in a wide range of radiographic abnormalities. Multiple myeloma remains incurable.
Multiple myeloma accounts for one of the Ms in the popular mnemonic for lucent bone lesions FEGNOMASHIC.
On this page:
Article:
Terminology
Diagnosis
Epidemiology
Clinical presentation
Pathology
Radiographic features
Treatment and prognosis
Differential diagnosis
Related articles
References
Images:
Cases and figures
Imaging differential diagnosis
Terminology
As per the WHO classification of tumors of hematopoietic and lymphoid tissues, multiple myeloma is called plasma cell myeloma 14. Historically, it was sometimes known as Kahler disease or myelomatosis 13.
Four main patterns are recognized:
disseminated form: multiple well-defined "punched out" lytic lesions: predominantly affecting the axial skeleton
disseminated form: diffuse skeletal osteopenia
solitary plasmacytoma: a single large/expansile lesion most commonly in a vertebral body or in the pelvis
osteosclerosing myeloma
The remainder of this article relates to the disseminated forms. Please refer to the article plasmacytoma for discussion of the latter.
Smoldering multiple myeloma refers to a form that falls on the spectrum between monoclonal gammopathy of unknown significance (MGUS) and active multiple myeloma. Patients are asymptomatic, with worse biochemistry than MGUS but without the end-organ damage of active multiple myeloma 9.
Diagnosis
International Myeloma Working Group updated criteria for the diagnosis of multiple myeloma has following definition for multiple myeloma 15:
clonal bone marrow plasma cells ≥10% or biopsy-proven bony or extramedullary plasmacytoma, and
any one or more of the following myeloma defining events:
evidence of end-organ damage that can be attributed to the underlying plasma cell proliferative disorder, specifically:
hypercalcemia: serum calcium >0.25 mmol/L (>1 mg/dL) higher than the upper limit of normal or >2.75 mmol/L (>11 mg/dL)
renal insufficiency: creatinine clearance <40 mL per min or serum creatinine >177 μmol/L (>2 mg/dL)
anemia: hemoglobin value of >20 g/L below the lower limit of normal, or a hemoglobin value <100 g/L
bone lesions: one or more osteolytic lesions on skeletal radiography, CT, or PET-CT
any one or more of the following biomarkers of malignancy
clonal bone marrow plasma cell percentage ≥60%
involved:uninvolved serum free light chain ratio ≥100
1 focal lesions on MRI studies
The myeloma defining events can be recalled with the mnemonic SLiM-CRAB 15.
Epidemiology
Multiple myeloma is a common malignancy in patients above 40; 70% of cases are diagnosed between ages 50 and 70 with a median age of diagnosis being 70 years; there is a male predilection (M: F 2:1) 7,12,14. It accounts for 1% of all malignancies and 10-15% of all hematological neoplasms 12,14. Black populations are affected at nearly twice the rate as White populations 14. Multiple myeloma and osteosarcoma combined account for ~50% of all primary bone malignancies 7.
Clinical presentation
Clinical presentation of patients with multiple myeloma is varied, and includes 1,2,7:
bone pain
initially intermittent, but becomes constant
worse with activity/weight-bearing, and thus is worse during the day
anemia
typically normochromic/normocytic
renal failure
hypercalcemia
proteinuria
The typical features can be recalled with the mnemonic CRAB 12.
Complications
Presentation may also be with acomplication, including:
pathological fracture
vertebral compression fracture
long bone fracture (e.g. proximal femur)
amyloidosis
recurrent infection: e.g. pneumonia due to leukopenia
plasmacytomas typically progress to multiple myeloma
Pathology
Multiple myeloma results from monoclonal proliferation of malignant plasma cells which produce immunoglobulins and infiltrate haemopoietic locations (i.e. red marrow). The paraprotein produced is most commonly IgG (~50%), followed by IgA (~20%) and light chain only (~15%), while IgM and non-secretory multiple myeloma are very rare 17.
Renal involvement is common and renal failure is multifactorial:
obstructive casts form in the renal tubules composed of Bence Jones proteins, immunoglobulins, albumin and Tamm-Horsfall proteins
most common cause of renal failure in multiple myeloma
direct nephrotoxicity of Bence Jones proteins on the epithelial cells of the renal tubules
hypercalcemia and dehydration
hyperuricemia and urate nephropathy due to high cell turnover
amyloidosis (AL type)
increased risk of renal infection
The initial presentation occasionally is a polyneuropathy when it is part of POEMS syndrome (mostly the sclerotic form).
Markers
reverse albumin/globulin ratio (i.e. low albumin, high globulin)
monoclonal gammopathy (IgA and/or IgG peak)
Bence Jones protein (Ig light chain) proteinuria
hypercalcemia
decreased or normal alkaline phosphatase (ALP) unless there is a pathological fracture due to impaired osteoblastic function
Approximately 3% of cases will have a negative serum electrophoresis (i.e. non-secretory MM) 16 and negative urine Bence Jones protein ref.
Staging
The most popular staging system, the International Staging System, uses the combination of β2-microglobulin test and serum albumin 6.
Distribution
Distribution of multiple myeloma mirrors that of red marrow in the older individual, and thus this is mostly encountered in the axial skeleton and proximal appendicular skeleton 14:
vertebrae (most common)
ribs
skull
shoulder girdle
pelvis
long bones
extraskeletal structures (extraosseous myeloma): rare
Radiographic features
Radiology has a number of roles in the diagnosis and management for multiple myeloma:
suggest the diagnosis / exclude other causes
assess possible mechanical complications (e.g. pathological fracture)
assess disease progression
Disseminated multiple myeloma has two common radiological appearances, although it should be noted that initially, radiographs may be normal, despite the presence of symptoms. The two main diffuse patterns are 12:
numerous, well-circumscribed, lytic bone lesions (70% of cases 14)
punched out lucencies
raindrop skull 7
endosteal scalloping
generalized osteopenia (less common)
often associated with vertebral compression fractures/vertebra plana
Plain radiograph
A skeletal survey is essential not only for the diagnosis of multiple myeloma but also in pre-empting potential complications (e.g. pathological fracture) and assessing response to therapy. ~40% bone destruction is required for lesion detection, thus giving the skeletal survey a high false-negative rate of ~50% (range 30-70%) 12.
The vast majority of lesions are purely lytic, sharply defined/punched out, with endosteal scalloping when abutting the cortex. Lesions are sclerotic in only 3% of patients 7.
CT
Whole-body low dose CT is more accurate than a skeletal survey with a sensitivity of ~70% and specificity of ~90% with a dose 1-2x that of a skeletal survey 12. Whole-body low dose CT is also better to assess the risk of pathological fracture in severely affected bones as well as the presence of extramedullary lesions 12.
MRI
A whole-body MRI technique may be deployed. MRI is more sensitive in detecting multiple lesions compared to the standard plain film skeletal survey and CT 8,12. Five patterns have been described 12:
normal bone marrow signal
diffuse involvement
focal involvement
combined diffuse and focal involvement
variegated ("salt and pepper")
Signal characteristics
Most frequently used MR sequences for the evaluation of bone marrow are conventional T1 spin-echo and T2 spin-echo sequences 11.
T1
typically low signal
high-grade, diffuse involvement may become isointense to adjacent normal marrow
T2 with fat-suppression
high signal
infiltration of the ribs is probably best appreciated on T2 images with fat suppression, appearing bright: ‘white ribs sign’
T1 C+ (Gd)
hyperintense
several enhancement curves may be seen:
type 4 curve: represents a steep wash-in of contrast medium, due to the high vascularization and perfusion with leakage through the highly permeable capillaries, followed by an early wash-out back into the intravascular space because of the small interstitial space with closely packed plasma cells 10,11
type 3 and type 5 curves may also be seen
DWI/ADC: lesions usually exhibit restricted diffusion, with higher signal on high b-value DWI compared to the very low signal of normal background marrow 11
Nuclear medicine
Bone scintigraphy
Bone scintigraphy appearances of disseminated multiple myeloma is variable due to the potential lack of osteoblastic activity. Larger lesions may be either hyperactive (hot) or photopenic (cold). Bone scans may also be normal. Therefore, bone scans usually do not contribute significant information to the workup of patients with suspected or established disseminated multiple myeloma, as the sensitivity of detecting lesions is less than that of a plain film skeletal survey 7.
FDG PET-CT
FDG PET-CT is effective in identifying the distribution of disease 14. F-18 FDG uptake by the myeloma lesions corresponds to lytic bone lesions or soft tissue plasmacytomas seen on CT. However, focal high FDG uptake in the bone may be considered a positive lesion even in the absence of osteolysis on CT.
Treatment and prognosis
Multiple myeloma remains incurable with a median survival of 5.5 years (range <6 months to >10 years) 14. Management with agents such as thalidomide, lenalidomide, bortezomib (proteasome inhibitor), and daratumumab (CD38 monoclonal antibody) have provided significant survival gains 6. These are typically used in combination with older agents such as cyclophosphamide, melphalan, or dexamethasone 6.
Stem-cell harvest and autologous hematopoietic stem cell transplant post-chemotherapeutic/radiotherapy bone marrow ablation are also used, although relapse is inevitable.
Response assessment
As imaging is not required to diagnose multiple myeloma, assessment of treatment response does not necessitate imaging studies, with the exception of so-called "imaging plus minimal residual disease negative" status, which requires FDG PET. However, patients who have known lesions identified on radiologic studies of various modalities at baseline should have these reevaluated as part of response assessment. See the separate article on the International Myeloma Working Group response criteria.
Complications
crystal-storing histiocytosis
Differential diagnosis
The main differential is that of widespread bony metastases. Findings that favor the diagnosis of bone metastases over that of multiple myeloma include:
more commonly affect the vertebral pedicles rather than vertebral bodies
distal appendicular skeleton
although both entities have variable bone scan appearances (both hot and cold) unlike myeloma, extensive bony metastases rarely have a normal appearance
Other rare entities include:
Waldenström macroglobulinemia: IgM paraprotein
Quiz questions
Question 3178
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An 80 year old woman undergoes skull radiography (below) after a fall. What is the likely etiology for the X-ray finding?
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References
Wolfgang Dähnert. Radiology Review Manual. (2003) ISBN: 9780781738958 - Google Books
Ralph Weissleder. Primer of Diagnostic Imaging. (2007) ISBN: 9780323040686 - Google Books
Hanrahan C, Christensen C, Crim J. Current Concepts in the Evaluation of Multiple Myeloma with MR Imaging and FDG PET/CT. Radiographics. 2010;30(1):127-42. doi:10.1148/rg.301095066 - Pubmed
Delorme S & Baur-Melnyk A. Imaging in Multiple Myeloma. Eur J Radiol. 2009;70(3):401-8. doi:10.1016/j.ejrad.2009.02.005 - Pubmed
Roodman G. Skeletal Imaging and Management of Bone Disease. Hematology Am Soc Hematol Educ Program. 2008;2008(1):313-9. doi:10.1182/asheducation-2008.1.313 - Pubmed
Advances in Malignant Hematology. (2011) - Google Books
Terry R. Yochum, Lindsay J. Rowe. Essentials of Skeletal Radiology. (2005) ISBN: 9780781739467 - Google Books
Peter Reimer, Paul M. Parizel, James F.M. Meaney et al. Clinical MR Imaging. (2010) ISBN: 9783540745013 - Google Books
Dispenzieri A, Stewart A, Chanan-Khan A et al. Smoldering Multiple Myeloma Requiring Treatment: Time for a New Definition? Blood. 2013;122(26):4172-81. doi:10.1182/blood-2013-08-520890 - Pubmed
Baur-Melnyk A, Buhmann S, Dürr H, Reiser M. Role of MRI for the Diagnosis and Prognosis of Multiple Myeloma. Eur J Radiol. 2005;55(1):56-63. doi:10.1016/j.ejrad.2005.01.017 - Pubmed
Dutoit J & Verstraete K. MRI in Multiple Myeloma: A Pictorial Review of Diagnostic and Post-Treatment Findings. Insights Imaging. 2016;7(4):553-69. doi:10.1007/s13244-016-0492-7 - Pubmed
Ormond Filho A, Carneiro B, Pastore D et al. Whole-Body Imaging of Multiple Myeloma: Diagnostic Criteria. Radiographics. 2019;39(4):1077-97. doi:10.1148/rg.2019180096 - Pubmed
Kyle R & Rajkumar S. Multiple Myeloma. Blood. 2008;111(6):2962-72. doi:10.1182/blood-2007-10-078022 - Pubmed
WHO Classification of Tumours Editorial Board. Soft Tissue and Bone Tumours. (2020) ISBN: 9789283245025 - Google Books
Rajkumar S, Dimopoulos M, Palumbo A et al. International Myeloma Working Group Updated Criteria for the Diagnosis of Multiple Myeloma. Lancet Oncol. 2014;15(12):e538-48. doi:10.1016/s1470-2045(14)70442-5
Chang W, Koh H, Yoon S, Kim H, Eom K, Kim I. The Predictive Value of Serum Myeloma Protein in Solitary Plasmacytoma. Radiat Oncol J. 2020;38(2):129-37. doi:10.3857/roj.2019.00570 - Pubmed
Kyle R, Gertz M, Witzig T et al. Review of 1027 Patients with Newly Diagnosed Multiple Myeloma. Mayo Clin Proc. 2003;78(1):21-33. doi:10.4065/78.1.21 - Pubmed
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Radiolucent lesions of the mandible (differential)
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Permeative process in bone
Lucent/lytic skull lesions (mnemonic)
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Plasmacytoma - pelvic bone
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Multiple myeloma
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Multiple myeloma
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Related articles: Bone tumours
The differential diagnosis for bone tumors is dependent on the age of the patient, with a very different set of differentials for the pediatric patient.
bone tumors
bone-forming tumors[+][+]
adamantinoma of long bones
enostosis (bone island)
exostosis
subungual exostosis
turret exostosis
osteoid osteoma
osteoblastoma
osteopoikilosis
osteoma
paranasal sinus osteoma
skull vault osteoma
osteosarcoma
conventional osteosarcoma
telangiectatic osteosarcoma
small cell osteosarcoma
periosteal osteosarcoma
parosteal osteosarcoma
string sign
high-grade surface osteosarcoma
secondary osteosarcoma
cartilage-forming tumors[+][+]
bizarre parosteal osteochondromatous proliferation (Nora lesion)
chondroblastoma
chondromyxoid fibroma
chondrosarcoma
conventional chondrosarcoma
central ACT/CS1
central chondrosarcomagrade 2 and 3
secondary peripheral ACT/CS1
secondary peripheral chondrosarcoma grade 2 and 3
periosteal chondrosarcoma
clear cell chondrosarcoma
myxoid chondrosarcoma
mesenchymal chondrosarcoma
dedifferentiated chondrosarcoma
extraskeletal chondrosarcoma
enchondroma
enchondroma vs low grade chondrosarcoma
enchondromatosis (Ollier disease)
Maffucci syndrome
juxtacortical chondroma
osteochondroma
hereditary multiple exostoses
dysplasia epiphysealis hemimelica (Trevor disease)
fibrous bone lesions[+][+]
desmoplastic fibroma
fibrosarcoma of bone
fibrous dysplasia
Mazabraud syndrome
McCune-Albright syndrome
rind sign
liposclerosing myxofibrous tumor (LSMFT)
malignant fibrous histiocytoma (MFH)
ossifying fibroma
fibroxanthoma
fibrous cortical defect
non-ossifying fibroma
bone marrow tumors
Ewing sarcoma
Langerhans cell histiocytosis
multiple myeloma
primary bone lymphoma
secondary bone lymphoma
solitary bone plasmacytoma
solitary bone plasmacytoma with minimal bone marrow involvement
other bone tumors or tumor-like lesions[+][+]
adamantinoma
aneurysmal bone cyst
benign fibrous histiocytoma
chordoma
giant cell tumor of bone
paint brush borders sign
Gorham massive osteolysis
hemangioendothelioma
musculoskeletal hemangioendothelioma
hemophilic pseudotumor
intradiploic epidermoid cyst
intraosseous lipoma
cockade sign
musculoskeletal angiosarcoma
musculoskeletal hemangiopericytoma
primary intraosseous hemangioma
post-traumatic cystic bone lesion
simple bone cyst
skeletal metastases[+][+]
morphology
blow out bone metastases
cookie bite skeletal metastases
lytic bone metastases
mixed lytic and sclerotic bone metastases
sclerotic bone metastases
location
epiphyseal lesions (mnemonic)
diaphyseal lesions (mnemonic)
metaphyseal lesions
distal appendicular skeletal metastases
skull metastases
patellar tumors
vertebral metastases
impending fracture risk
Harrington criteria
Mirel classification
staging[+][+]
AJCC staging of musculoskeletal tumors
Enneking surgical staging system
approach[+][+]
describing a bone lesion
Lodwick classification of lytic bone lesions
Modified Lodwick-Madewell classification of lytic bone lesions
differentials
lucent/lytic bone lesion
solitary well defined osteolytic lesion
solitary ill-defined osteolytic lesions
multiple lucent/lytic bone lesions
lucent/lytic rib lesion
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Cases and figures
Figure 1: illustration - distribution of multiple myeloma
Case 1: with raindrop skull
Case 2
Case 3: MRI T1
Case 4: endosteal scalloping
Case 5
Case 6
Case 7
Case 8: T1 C+
Case 9: involving orbit
Case 10: with pathological fractures
Case 11
Case 12
Case 13: with vertebra plana
Case 14
Case 15
Case 16
Case 17
Case 18
Case 19
Case 20
Case 21: involving skull base
Case 22: with generalized osteopaenia
Case 23
Case 24
Case 25
Case 26
Case 27
Case 28
Case 29
Case 30
Case 32
Case 31: raindrop skull
Case 33: osteosclerosing myeloma
Case 34: scapular and clavicular
Case 35: disseminated
Case 36
Case 37: thumb
Case 38
Imaging differential diagnosis
Osseous metastases from breast cancer
© 2005–2025 Radiopaedia.org |
11327 | http://webspace.ship.edu/mrcohe/inside-out/vu1/d_joyce/elements/bookI/guide2.html | Euclid's Elements, Book I, Guide
On Propositions I.4 through I.8
This next group of propositions includes two congruence propositions for triangles, I.4 and I.8, and two propositions about isosceles triangles, I.5 and I.6. Proposition I.7 is only used in I.8 and could have been made part of I.8, but was probably separated in order to reduce the length of the proof in I.8.
Proposition I.4
If two triangles have two sides equal to two sides respectively, and have the angles contained by the equal straight lines equal, then they also have the base equal to the base, the triangle equals the triangle, and the remaining angles equal the remaining angles respectively, namely those opposite the equal sides.
This is the familiar side-angle-side congruence proposition for triangles. When two triangles have two sides and the included angle equal, then the remaining sides, angle, and area are also equal, that is to say, they're congruent. Symbolically, given triangles ABC and DEF with AB = DE, AC = DF, and angle BAC = angle EDF, then the rest of the parts of the triangles are the same.
Euclid's proof of this proposition relies on the "principle of superposition". This principle is not supported by his postulates, and so it would be more appropriate to take I.4 as a postulate than pretend that it is adequately justified by its proof. For more discussion on this point, see the Guide for I.4.
There will be two other congruence propositions: I.8, side-side-side, and I.26, side and two angles.
Proposition I.5
In isosceles triangles the angles at the base equal one another, and, if the equal straight lines are produced further, then the angles under the base equal one another.
An isosceles triangle is defined in I.Def.20 as a triangle with two equal sides. In the figure AB = AC, so triangle ABC is isosceles. One of the properties of such triangles is that they also have two equal angles, the base angles of the triangle, angles ABC and ACB. That's the first part of the statement of Proposition I.5. The other conclusion is that the angles supplementary to the base angles are also equal, that is, angles DBC and ECB are equal.
Guide to Book I, continued
Previous page of the Guide
Book I Introduction
© 1999
D.E.Joyce
Clark University |
11328 | https://www.federalreserve.gov/econres/notes/feds-notes/the-interaction-of-bank-leverage-interest-rate-risk-and-runnable-funding-20240830.html | The Fed - The interaction of bank leverage, interest rate risk, and runnable funding
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August 30, 2024
The interaction of bank leverage, interest rate risk, and runnable funding
Shawn Kimble and Matthew P. Seay1
Summary
Silicon Valley Bank (SVB), Signature Bank, First Republic Bank (FRC) had too little useable liquidity relative to their runnable funding and too little capital given the magnitude of their interest rate risk. The mismanagement of these vulnerabilities ultimately contributed to a loss of confidence in their business models. While SVB, Signature, and FRC were outliers, we analyze the build-up of fragilities in the banking system that preceded their failures.
In this Note, we introduce a measure called lower friction liquidity (LFL). LFL is the ratio of liquid, useable assets (cash and useable available-for-sale (AFS) securities) to runnable liabilities (uninsured deposits and short-term wholesale funding (STWF)). Useable AFS is defined as the maximum amount of AFS a firm can liquidate to meet outflows without breaching its total common equity tier 1 (CET1) ratio requirement. We also construct market-adjusted common equity tier 1 (MACET1) ratios to account for unrealized fair value losses on all bank securities and loans in bank capital ratios. We use these two measures to analyze the interaction of banks' liquidity and solvency risks.
While there is no perfect measure of bank capital or liquidity, LFL captures banks' capacity to meet outflows using assets that are easily convertible to cash while maintaining regulatory capital requirements. It assumes severe financial conditions, similar to those that prevailed during the spring of 2023, in which vulnerable banks cannot rely on funding markets to shore up their cash positions and are unable to raise equity.
In this Note, we decompose the subcomponents of LFL ratios and show that in the year leading up to the failure of SVB, banks with lower LFL ratios shed more cash than their peers and retained fewer AFS securities, despite a comparable build in uninsured deposits. Following the failure of SVB, banks with low LFL ratios had worse stock price returns than their peers – suggesting that markets overlooked this interaction of vulnerabilities until the firm failed. In addition, firms with low LFL ratios displayed less ability to retain their uninsured depositors following SVB's collapse, despite significantly boosting their useable, liquid asset positions.
Our analysis highlights that firms in the bottom quartile of the LFL ratio distribution could cover just one-third of their runnable funding by selling their most useable, liquid assets. In general, large fair value losses can impair the usability of high duration liquid assets should funding stress emerge.2 For the subset of otherwise solvent institutions with viable business models but too little useable liquidity, discount window readiness or access to contingent liquidity facilities could provide balance sheet flexibility and delay or mitigate potential bank failures and contagion.3 For the subset of firms that operate with sufficient liquidity but elevated interest rate risk, more capital could also help stave-off a run equilibrium.4
Limited ability to sell assets without depleting capital
Fragilities began to build in the banking system several years prior to SVB's collapse. From 2020 to 2022, banks invested heavily in longer-maturity securities and loans (figure 1, left). At the time, yields on these assets were low relative to current levels, but offered a premium relative to short-term investments. Higher reliance on longer-maturity assets left some banks' capital positions increasingly vulnerable to higher long-term yields. That vulnerability manifested during 2022, when inflation unexpectedly rose, which corresponded with a large rise in long-term yields, and led to substantial reductions in the fair value of fixed-rated bank loans and securities.
To illustrate the impact of these unrealized losses on banks' regulatory capital, we construct MACET1 ratios. The MACET1 ratio is a non-regulatory risk-based measure of capital that accounts for fair value losses of all securities and loans.5 MACET1 ratios illustrate that bank capital would be significantly depleted in an extreme scenario where fair value losses are realized (figure 1, right).6
Figure 1. Longer maturity assets and lower capital
Note: Left panel is an approximation of the repricing and maturity distribution of bank assets through time. The distribution is based on estimates of individual bank's asset maturity, which are constructed by balance-weighting the midpoint of each repricing and maturity bucket from the distribution loans and securities in Call Reports. Right panel includes most publicly-traded banks, which represent about two-thirds of banking system assets. MACET1 ratios are equal to CET1 ratios less fair value losses on all securities and loans. Securities fair value losses are sourced from FR Y-9C and Call Reports. Loan fair value losses are sourced from S&P Global Capital IQ Pro.
Source: FR Y-9C, Call Reports, S&P Global Capital IQ Pro, Author Calculations.
Accessible version
Imbalance of runnable funding and useable, liquid assets
Uninsured deposits increased substantially as the federal response to the pandemic made its way into the banking system during 2020. At an aggregate level, this growth of runnable funding was mostly matched with higher cash positions (including reserves) and larger holdings of AFS through 2021 (figure 2). As the pandemic waned and the Fed tightened monetary policy, the quantity of reserves in the banking system shrank. In addition, some banks reduced their AFS portfolios, despite maintaining a high reliance on uninsured deposits. This imbalance of runnable funding relative to useable, liquid assets peaked during the second half of 2022 and left a subset of banks less equipped to meet deposit outflows without either increasing reliance on repo market depth, turning to other funding sources such as Federal Home Loan Banks (FHLBs), or using the discount window (DW).7
Figure 2. Components of useable liquid assets and runnable liabilities
Note: Includes all banks with at least $1 billion in assets.
Source: FR Y-9C and Call Reports.
Accessible version
Lower friction liquidity: the interaction of runnable funding, interest rate risk, and leverage
While many firms had sufficient asset-liquidity to meet the runnability of their liability base, some banks failed to correct this imbalance and adequately manage the interaction of their risks. LFL ratios provide one way to analyze bank resiliency based on the interaction of a bank's liquidity, interest rate risk, and capital positions. Banks with lower LFL ratios have less liquidity immediately available to manage higher cash demand from their depositors and short-term lenders without increasing borrowings and have less flexibility to shrink their balance sheets without raising more capital.8
More formally, LFL is the ratio of banks' useable, liquid assets to their runnable liabilities. We define useable, liquid assets as cash (including reserves) and useable AFS, where useable AFS is the maximum amount of AFS securities a firm can liquidate to meet outflows without breaching its total CET1 capital requirement.9 We assume that banks sell each dollar of securities at a loss rate equivalent to the average fair value decline of the AFS portfolio.10,11
Runnable liabilities – the denominator of LFL ratios – are the sum of uninsured deposits and short-term wholesale funding (STWF), where STWF is the sum of federal funds borrowing, repurchase agreements, foreign deposits, trading liabilities, other borrowings with a remaining maturity < 1-year, commercial paper, and long-term debt scheduled to mature < 1-year. The measure assumes a system-wide run. Under this extreme assumption, banks have no ability to retain their uninsured deposits.
The left panel of figure 3 shows that banks' ability to meet runnable funding outflows – as measured by LFL ratios – rose gradually during 2018 to 2019. During the early stages of the pandemic, LFL ratios were bolstered by significant holdings of AFS securities and reserves. LFL ratios declined materially during 2022, as uninsured deposits remained fairly sticky while cash and reserve positions declined as the Fed tightened, and securities portfolios shifted toward held-to-maturity. This imbalance is demonstrated by the leftward shift in the distribution of firms' LFL ratios, as shown in the right panel of figure 3.
Figure 3. Distribution of LFL Ratios
Note: LFL is the ratio of cash and useable AFS securities to uninsured deposits and other runnable funding. Both charts include panel of banks with at least $1 billion in assets. The right panel is trimmed to show banks with LFL ratios less than 2.
Source: FR Y-9C, Call Reports, and Author calculations.
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How did runnable funding and liquidity evolve before and after the failure of SVB?
We next analyze how each of the LFL components (cash, useable AFS, uninsured deposits, and STWF) contributed to changes in banks' LFL ratios. We group banks into two categories based on the level of their LFL ratios as of 2022:Q4. Banks with LFL ratios less than 0.33 – roughly the bottom quartile of the distribution at that time – are grouped in the low LFL group, and all other banks are grouped in the high LFL group. We drop failed banks and exclude GSIBs.12 We then create virtual, aggregate banks to represent the high and low LFL bank groups. We sum the data at the LFL component level each quarter across the individual banks in the group, and then create a single quarterly LFL measure from those aggregated data. This approach allows us to calculate percentage-point contributions to the quarterly change in each bank group's aggregate LFL ratio from each of our four LFL components and contrast how their positions evolved. On a quarterly basis, the four contribution amounts sum to the total change in our LFL measure. Figure 4 plots the contribution of each of our four components for each quarter. Data for the low LFL bank group are shown in the left panel, and those for the high LFL bank group are shown in the right panel.
Figure 4. LFL Decomposition for Low and High LFL Banks
Note: Includes balanced panel of banks with at least $1 billion in assets excluding GSIBs.
Source: FR Y-9C, Call Reports, and Author calculations.
Accessible version
The figures show the large influx of uninsured deposits across low and high LFL bank groups during 2020 and early 2021. During this time, both high and low LFL banks largely matched inflows of uninsured deposits with cash and AFS securities. Beginning in late 2021 and through 2022, low LFL banks shed significantly more cash and AFS securities despite maintaining high levels of uninsured deposits, which led to a material reduction in their ability to meet outflows. In contrast, firms with healthier LFL ratios maintained more of their useable liquidity through 2022. After SVB's failure, low LFL banks shored up significantly more liquidity by increasing their cash positions and moving toward AFS securities.13
When did markets price the interaction of interest rate risk and runnable funding?
While the largest banks are subject to more stringent regulatory requirements, such as the GSIB surcharge or the liquidity coverage ratio, any firm that severely mismanages its interest rate risk or funding positions, or their interaction, may face market discipline or heightened attention from depositors.
Figure 5 plots the simple average of cumulative stock price returns for low LFL banks (LFL ratio < .33) and all other firms (LFL ratios > .33). The chart suggests markets priced the interaction of vulnerabilities captured by low LFL ratios after the failure of SVB.14 Furthermore, the similar cumulative returns across both bank groups before the failure of SVB suggest evidence of parallel trends.
Figure 5. Cumulative returns by LFL group
Note: LFL is the ratio of cash and useable AFS securities to uninsured deposits and other runnable funding. Chart shows the simple average of cumulative returns by LFL grouping. Sample includes 293 publicly traded banks.
Source: FR Y-9C, Call Reports, S&P Global Market Intelligence, and Author Calculations..
Accessible version
We use cross-sectional analysis to explore this more formally. We assume market participants are informed by the latest available balance sheet information at the time of SVB's failure and use 2022:Q4 balance sheets to identify banks with similar vulnerabilities.15 Table 1 shows cumulative returns from March 8th to May 31st regressed on several vulnerability measures. The main variable of interest that separates the treatment and control in our specifications is a dummy variable which takes the value of 1 if a firm has a LFL ratio below 0.33 (within the bottom quartile of the distribution). Column (1) shows that banks with ex-ante vulnerability, with low LFL ratios as of 2022:Q4, underperformed their peers after the failure of SVB. In Column (2) we add two additional controls related to interest rate risk and runnable funding. We add a dummy variable set equal to 1 for firms with MACET1 ratios less than their total CET1 requirement. This control is designed to capture firms that may need to raise equity to cover interest rate risk stemming from securities and loans (FV losses) in the event of a severe bank run. We add a separate control for runnable funding using a dummy variable equal to 1 for firms with above-average reliance on uninsured deposits. Our findings suggest that low LFL ratios are associated with worse stock price performance after SVB's failure, above what can be gleaned from interest rate risk and runnable funding individually.
Column (3) includes a dummy variable for firms with MACET1 ratios less than 4.5 percent. Banks with CET1 ratios less than 4.5 percent are considered undercapitalized by PCA standards. While MACET1 is not a regulatory capital measure, we apply the 4.5 percent as a solvency threshold to identify potentially vulnerable banks with too little capital relative to their interest rate risk and its interaction with above-average reliance on uninsured deposits. Our results are robust to these controls. Stock prices of banks with low LFL ratios underperformed their peers by 6.7 percentage points on average after the failure of SVB, as shown in Column (3) of table 1. This suggests market participants may have weighed banks' ability to meet deposit outflows in the short-term, and the interaction of solvency and runnable funding, similarly.
Table 1: Cumulative returns by LFL group
| | (1) | (2) | (3) |
---
| LFL Ratio < Bottom quartile | -0.077 | -0.067 | -0.067 |
| (0.015) | (0.016) | (0.015) |
| MACET1 Ratio < Total CET1 Req. | | -0.059 | -0.049 |
| | (0.013) | (0.014) |
| Uninsured Reliance > Avg. | | -0.021 | -0.010 |
| | (0.014) | (0.015) |
| MACET1 Ratio < 4.5 | | | 0.002 |
| | | (0.035) |
| Uninsured Reliance > Avg. & MACET1 Ratio < 4.5 | | | -0.069 |
| | | (0.039) |
| Obs. | 296 | 296 | 296 |
| Adj. R-squared | 0.073 | 0.138 | 0.153 |
| Fixed effects | No | No | No |
Note: Cumulative bank stock price returns are the outcome variable. All control variables use balance sheet data as of 2023:Q4. LFL is the ratio of cash and useable AFS securities to uninsured deposits and other runnable funding. Banks with LFL ratios below 0.33 are in the bottom quartile of the LFL ratio distribution. MACET1 ratios incorporate fair value losses for all securities and loans on bank CET1 ratios. Total CET1 requirements are based on individual bank capital requirements for stress tested firms. For all others, we assume a total CET1 requirement of 7 percent. The sample excludes failed banks and GSIBs. Cumulative returns are calculated from March 8 th to May 31 st, 2023. Results are shown with robust standard errors. Significance: p < 0.1, p < 0.05, p < 0.01.
Source: FR Y-9C, Call Reports, and S&P Global Capital IQ Pro.
Did banks with larger imbalances of liquid assets to runnable funding have bigger uninsured deposit outflows?
Next, using similar cross-sectional analysis, we test whether banks with LFL ratios < 0.33 experienced larger uninsured deposit outflows relative to their peers following the SVB shock.16
We find that banks with low LFL ratios had roughly 8.2 percentage points less average quarterly uninsured deposit growth than their peers after the failure of SVB (Table 2, Column 1). Further, we show in Columns (2) and (3) that our uninsured deposit growth estimate is still economically and statistically significant after controlling for above-average reliance on uninsured deposits and MACET1 ratios less than 4.5 percent. These findings are consistent with the hypothesis that banks with an unmatched reliance on uninsured deposits (captured via lower LFL ratios, all else held equal), are likely to have greater difficulty in maintaining or attracting a stable deposit base.
Table 2: Uninsured deposit growth by LFL group
| | (1) | (2) | (3) |
---
| LFL Ratio < Bottom quartile | -0.082 | -0.055 | -0.055 |
| (0.011) | (0.010) | (0.010) |
| Uninsured Reliance > Avg. | | -0.098 | -0.105 |
| | (0.012) | (0.015) |
| MACET1 Ratio < 4.5 | | | -0.030 |
| | | (0.026) |
| Uninsured Reliance > Avg. # MACET1 Ratio < 4.5 | | | 0.022 |
| | | (0.027) |
| Obs. | 733 | 733 | 733 |
| Adj. R-squared | 0.027 | 0.094 | 0.095 |
| Fixed effects | No | No | No |
Note: Average quarterly change in uninsured deposits from 2022:Q4 through 2023:Q2 is the outcome variable. All control variables use balance sheet data as of 2022:Q4. LFL is the ratio of cash and useable AFS securities to uninsured deposits and other runnable funding. Banks with low LFL ratios are defined as those with LFL ratios below 0.33 as of 2022:Q4. Deposit growth is winsorized at the 99th percentile. Excludes GSIBs and failed banks. Results are shown with robust standard errors. Significance: p < 0.1, p < 0.05, p < 0.01.
Source: FR Y-9C, Call Reports, and S&P Global Capital IQ Pro.
Conclusion
In this note we introduce a new measure called lower friction liquidity (LFL), which is the ratio of a banks' most useable, liquid assets to their most runnable liabilities. LFL ratios provide a way to highlight banks that have less ability to meet outflows of runnable funding based on their liquidity positions, interest rate risk, and capital positions. We provide some evidence that markets overlooked the interaction of these vulnerabilities until SVB failed. We also share some preliminary evidence that suggests banks with low LFL ratios had less ability to retain their uninsured deposits post-SVB, relative to their peers.
It is unlikely that the next set of bank failures will look like the last. However, our work suggests that otherwise solvent institutions with viable business models could better position their balance sheet to meet larger and faster outflows without significantly depleting their capital. Examples of such strategies include discount window readiness and access to other liquidity facilities. For firms with elevated interest rate risk but sufficient liquidity, more capital could also help prevent a run equilibrium.
References
Board of Governors of the Federal Reserve System (2023). Review of the Federal Reserve's Supervision and Regulation of Silicon Valley Bank (PDF). Washington: Board of Governors, April.
Caglio, Cecilia, Jennifer Dlugosz, and Marcelo Rezende. "Flight to safety in the regional bank crisis of 2023." Available at SSRN 4457140 (2023).
Choi, Dong Beom, Paul Goldsmith-Pinkham, and Tanju Yorulmazer. Contagion effects of the silicon valley bank run. No. w31772. National Bureau of Economic Research, 2023.
Cipriani, Marco, Thomas M. Eisenbach, and Anna Kovner. "Tracing Bank Runs in Real Time." FRB of New York Staff Report 1104 (2024).
Drechsler, Itamar, et al. "Banking on uninsured deposits." Available at SSRN 4411127 (2023).
Fischl-Lanzoni, Natalia, et al. "Investor Attention to Bank Risk During the Spring 2023 Bank Run." FRB of New York Staff Report 1095 (2024).
Flannery, Mark J., and Sorin M. Sorescu. "Partial effects of fed tightening on us banks' capital." Available at SSRN 4424139 (2023).
Glancy, David, et al. "The 2023 Banking Turmoil and the Bank Term Funding Program." (2024).
Haddad, Valentin, Barney Hartman-Glaser, and Tyler Muir. "Bank fragility when depositors are the asset." Available at SSRN 4412256 (2023).
Jiang, Erica Xuewei, et al. "Monetary tightening and US bank fragility in 2023: Mark-to-market losses and uninsured depositor runs?." Journal of Financial Economics 159 (2024): 103899.
Metrick, Andrew. "The failure of silicon valley bank and the panic of 2023." Journal of Economic Perspectives 38.1 (2024): 133-152.
1. Seay and Kimble are staff in the Division of Financial Stability at the Federal Reserve Board. The views in this Note are solely those of the authors and should not be interpreted as reflecting the views of the Board of Governors of the Federal Reserve System. We thank William Bassett, Skander Van den Heuvel, Chase Ross, Nathan Swem, Cindy Vojtech, and Phillip Weed for their helpful comments. Return to text
2. Agency mortgage-backed securities (MBS) are an example of a high duration, high quality liquid asset (HQLA). MBS are recorded at fair value in the liquidity coverage ratio, but if they are booked as held-to-maturity securities, fluctuations in their fair values have no impact on regulatory capital, as long as they are not sold. However, large declines in the fair value of securities can become a concern for banks facing liquidity pressures, in the event that they are forced to sell the securities and realize fair value losses. Selling HTM securities "taints" the entire portfolio and can weigh significantly on bank capital. Return to text
3. A diverse funding base can reduce the likelihood and severity of future deposit runs. For example, shifting business models toward less reliance on individual depositors with outsized deposit balances and toward diverse deposits across several industries are actions consistent with a more resilient funding model. Return to text
4. For further discussion on run rate equilibriums in an environment with rising rates see Drechsler et al. (2023), Haddad et al. (2023), Jiang et al. (2023). Return to text
5. See Flannery and Sorescu (2023) for additional estimates of fair value losses and their impact on bank capital for all call report filers. Return to text
6. All banks' regulatory capital positions are exempt from fair value losses on HTM securities and loans. MACET1 ratios do not adjust for the fair value of liabilities, which can also decrease as yields rise. For additional detail on how the value of deposits can change as yields rise, see Drechsler, Savov, Schnabel, and Wang (2023). Return to text
7. Banks pledge securities and loans to shore up liquidity. FR Y-9C or Call Reports contain total securities pledged, but do not provide a split of AFS and HTM pledged securities. Thus, for any bank that pledges AFS securities, LFL may overstate liquidity. Return to text
8. Consider the extreme case of SVB. Its deposit base was almost entirely uninsured, and it had invested heavily in high duration securities prior to the large increase in long-term yields, which left its market-adjusted equity negative in 2022. The firm failed after it announced a surprise capital raise of about $2 billion to cover losses that it had realized to meet the higher cash demand of its depositors. Tapping its HTM portfolio would exacerbate solvency concerns, and it was unprepared to secure additional borrowings quickly. Its failure demonstrated that interest rate risk mismanagement can severely limit the usability of high-quality assets – either by monetization or by selling outright. SVB had an LFL ratio of about 0.20 in the quarter prior to its failure, implying that it could cover just 20 percent of its runnable funding by liquidating cash and AFS securities. Similarly, FRC's LFL ratio was about 0.05 during 2022:Q4 – putting it in the bottom percentile of the LFL distribution. See Barr (2023) and Metrick (2023) for further details on SVB's failure. Return to text
9. All GSIBs can sell their entire AFS portfolios without breaching their capital requirements. GSIBs and other large banks have access to other sources of liquidity, such as their trading book, which enhances their liquidity positions beyond what is explored in this note. Return to text
10. Banks may loss minimize if they are forced sell a large portion of their securities holdings. Opaque data limit our ability to calculate LFL ratios with liquidation ordering, as Call Report data do not contain detailed information on the maturity distribution of unencumbered securities by security type. Return to text
11. During 2022:Q4, most firms could liquidate their entire AFS portfolio without breaching their total CET1 requirements. For the small set that could not, we maximize AFS sales by setting post-stress CET1 ratios equal to individual banks' total CET1 requirements. About one-fourth of banks would fall below their total CET1 requirements in the extreme scenario where they are forced to realize fair value losses on their HTM portfolios. Return to text
12. Caglio et al. (2023) show large banks' deposits increased after the failure of SVB, beyond what can be explained by reliance on uninsured deposits and fair value losses on securities. In addition, we exclude large banks' as they have additional levers to manage their liquidity that are not reflected in LFL ratios. Return to text
13. Cipriani et al. (2024) show that banks that endured runs bolstered their cash positions by increasing borrowings shortly after SVB's failure. Glancy et al. (2024) provide some evidence that banks that borrowed from the bank-term funding program had higher reliance on uninsured deposits and larger securities fair value losses on average. Return to text
14. Choi et al. (2023) highlight that investors appeared to price reliance on uninsured deposits, but not the realization of fair value losses, prior to the failure of SVB. Fischl-Lanzoni et al. (2024) also explore how investor attention on uninsured deposits and unrealized losses shifted after the run on SVB started. Return to text
15. There is roughly a 6-week lag separating quarter-end and the release of FR Y-9C and Call Report information. This would date the release of 2023 Q1 balance sheet information around the middle of May. Our sample ends May 31st. Return to text
16. We are interested in whether depositors were 'awakened' to these risks following SVB's failure. We focus on quantities rather than deposit pricing as presumably the decision faced by depositors' sudden concern for credit risk or loss of confidence, can be characterized as a binary decision between staying or fleeing, independent of the renumeration rate. Return to text
Please cite this note as:
Seay, Matthew P., and Shawn M. Kimble (2024). "The interaction of bank leverage, interest rate risk, and runnable funding," FEDS Notes. Washington: Board of Governors of the Federal Reserve System, August 30, 2024,
Disclaimer: FEDS Notes are articles in which Board staff offer their own views and present analysis on a range of topics in economics and finance. These articles are shorter and less technically oriented than FEDS Working Papers and IFDP papers.
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11329 | https://mathschallenge.net/library/number/perfect_numbers | mathschallenge.net
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Frequently Asked Questions
What are perfect, abundant, and deficient numbers?
The divisors of a natural number, excluding the number itself, are called the proper divisors . If the sum of proper divisors is equal to the number we call the number perfect. For example, the divisors of 28 are 1, 2, 4, 7, 14, and 28, so the sum of proper divisors is 1 + 2 + 4 + 7 + 14 = 28.
The first eight perfect numbers are 6, 28, 496, 8128, 33550336, 8589869056, 137438691328, 2305843008139952128.
If the sum of proper divisors exceeds the number it is called abundant (for example, 12: 1 + 2 + 3 + 4 + 6 = 16), and if the sum of proper divisors are less than the number it is called deficient (for example, 14: 1 + 2 + 7 = 10).
In number theory it is more convenient to define a perfect number as a number for which the sum of all its divisors is twice the number. We use the sum of divisors function, σ(n), to represent the sum of divisors of the natural number, n. So if P is a perfect number, σ(P)=2P.
The ancient Greeks knew that all the perfect numbers they discovered were of the form q×2 p−1, where p and q are prime.
For example, 6=3×2 2−1, 28=7×2 3−1, 496=31×2 5−1, 8128=127×2 7−1.
Although we have produced perfect numbers for p = 2, 3, 5, 7, it is not perfect when p = 11; the next cases work for p = 13, 17, 19, and then 31.
Leonhard Euler (1707-1783) was able to prove the conjecture: if a perfect number is even it WILL be of the form q×2 p−1, where q is prime. What no one has been able to prove is whether or not any odd perfect numbers exist.
By utilising the sum of divisor function, σ(n), we shall being by showing that if q is a prime of the form, 2 p−1, it will always be perfect.
Given the even number, P = q×2 p−1, where q is prime, we can then write,
σ(P) = σ(q×2 p−1) = σ(q)×σ(2 p−1) = (q+1)(2 p−1).
But if q is a prime of the form 2 p−1, we get,
σ(P) = (2 p−1+1)(2 p−1) = 2 p(2 p−1) = 2×2 p−1(2 p−1) = 2×q×2 p−1 = 2P.
Hence, if q is a prime of the form, 2 p−1, then the even number, P = q×2 p−1, will be perfect.
We shall now prove the converse...
Theorem
If P is an even perfect number it must be of the form P = 2 k−1(2 k−1).
Proof
Suppose that P is an even perfect number. All even numbers can be written in the form, q×2 k−1, where q is odd and k ³ 2.
Therefore, σ(P) = σ(q)×(2 k−1).
As P is perfect, σ(P) = 2P = q×2 k, and we can write, σ(q)×(2 k−1) = q×2 k. This leads to, σ(q) = q×2 k/(2 k−1).
Because σ(q) is integer, q must be divisible by 2 k−1, so let q = r(2 k−1), therefore, σ(q) = r×2 k.
As q is divisible by r, we know that its sum of divisors will at least be q+r. Therefore, σ(q) = r×2 k ³ q+r = r(2 k−1)+r = r(2 k−1+1) = r×2 k, which tells us that σ(q) = q+r. As q and r are the only divisors, q must be prime and r must be 1, hence q will be a prime of the form 2 k−1.
And so, if P is an even perfect, it will be of the form 2 k−1(2 k−1). Q.E.D.
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11330 | https://www.writersdigest.com/improve-my-writing/idealism-vs-realism | Idealism VS. Realism - Writer's Digest
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Idealism VS. Realism
The Daily Writer by Fred White It has been suggested that one is either an idealist or a realist (a variation on “one is either a Platonist or an Aristotelian”);…
Scott Francis
Published Oct 15, 2008 11:10 AM EDT
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The Daily Writer by Fred White
It has been suggested that one is either an idealist or a realist (a variation on “one is either a Platonist or an Aristotelian”); but of course the complex situations we encounter in daily life makes that adage seem a bit simplistic. There are times when we’re wildly idealistic and times when we see the world in an unrelentingly pragmatic, rational way, even though our temperament may orient us toward one or the other. In any case, it’s useful for writers to think about the effect that each attitude has on personality and behavior. Optimists tend to be adventurous, willing to try new things, to take risks, to put a lot of hope in potential; realists tend to settle for what is tried and true, always weighing the odds and making the safest bets. Most realists do not gamble. The odds of picking the winning numbers, they argue, are so great that there is virtually no difference between betting and not betting.
FOR FURTHER REFLECTION
Idealism (or optimism) and realism alike can suggest characters that exhibit one or the other personalities or world views. Jay Gatsby is the perennial romantic idealist and optimist, for example: even though Daisy had long ago rejected him and married another, he still believed he could have her. In Marquez’s Love in the Time of Cholera, the hero’s love for a woman he cannot attain lasts for fifty years. Love, paradoxically, is rooted in both ideal and realistic universes.
TRY THIS
Are you an idealist or a realist? Write a journal entry in which you answer that question.
Outline a short story in which a realist, through some fascinating series of circumstances, becomes an optimist—or vice versa.
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Scott FrancisAuthor
Scott Francis is a former editor and author of Writer's Digest Books.
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11331 | https://www.math.lsu.edu/~adkins/m2070/FourierSeries2015-1.pdf | Chapter 10 Fourier Series 10.1 Periodic Functions and Orthogonality Relations The differential equation 푦′′ + 훽2푦= 퐹cos 휔푡 models a mass-spring system with natural frequency 훽with a pure cosine forcing function of frequency 휔. If 훽2 ∕= 휔2 a particular solution is easily found by undetermined coefficients (or by using Laplace transforms) to be 푦푝= 퐹 훽2 −휔2 cos 휔푡.
If the forcing function is a linear combination of simple cosine functions, so that the differential equation is 푦′′ + 훽2푦= 푁 ∑ 푛=1 퐹푛cos 휔푛푡 where 훽2 ∕= 휔2 푛for any 푛, then, by linearity, a particular solution is obtained as a sum 푦푝(푡) = 푁 ∑ 푛=1 퐹푛 훽2 −휔2 푛 cos 휔푛푡.
This simple procedure can be extended to any function that can be repre-sented as a sum of cosine (and sine) functions, even if that summation is not a finite sum. It turns out that the functions that can be represented as sums in this form are very general, and include most of the periodic functions that are usually encountered in applications.
723 724 10 Fourier Series Periodic Functions A function 푓is said to be periodic with period 푝> 0 if 푓(푡+ 푝) = 푓(푡) for all 푡in the domain of 푓. This means that the graph of 푓repeats in successive intervals of length 푝, as can be seen in the graph in Figure 10.1.
푦 푝 2푝 3푝 4푝 5푝 Fig. 10.1 An example of a periodic function with period 푝. Notice how the graph repeats on each interval of length 푝.
The functions sin 푡and cos 푡are periodic with period 2휋, while tan 푡is periodic with period 휋since tan(푡+ 휋) = sin(푡+ 휋) cos(푡+ 휋) = −sin 푡 −cos푡= tan 푡.
The constant function 푓(푡) = 푐is periodic with period 푝where 푝is any positive number since 푓(푡+ 푝) = 푐= 푓(푡).
Other examples of periodic functions are the square wave and triangular wave whose graphs are shown in Figure 10.2. Both are periodic with period 2.
1 0 1 2 3 4 −1 푦 푡 (a) Square wave sw(푡) 1 0 1 2 3 4 5 −1 −2 푦 푡 (b) Triangular wave tw(푡) Fig. 10.2 10.1 Periodic Functions and Orthogonality Relations 725 Since a periodic function of period 푝repeats over any interval of length 푝, it is possible to define a periodic function by giving the formula for 푓on an interval of length 푝, and repeating this in subsequent intervals of length 푝.
For example, the square wave sw(푡) and triangular wave tw(푡) from Figure 10.2 are described by sw(푡) = { 0 if −1 ≤푡< 0 1 if 0 ≤푡< 1 ; sw(푡+ 2) = sw(푡).
tw(푡) = { −푡 if −1 ≤푡< 0 푡 if 0 ≤푡< 1 ; tw(푡+ 2) = tw(푡).
There is not a unique period for a periodic function. Note that if 푝is a period of 푓(푡), then 2푝is also a period because 푓(푡+ 2푝) = 푓((푡+ 푝) + 푝) = 푓(푡+ 푝) = 푓(푡) for all 푡. In fact, a similar argument shows that 푛푝is also a period for any positive integer 푛. Thus 2푛휋is a period for sin 푡and cos 푡for all positive integers 푛.
If 푃> 0 is a period of 푓and there is no smaller period then we say 푃is the fundamental period of 푓although we will usually just say the period. Not all periodic functions have a smallest period. The constant function 푓(푡) = 푐 is an example of such a function since any positive 푝is a period. The funda-mental period of the sine and cosine functions is 2휋, while the fundamental period of the square wave and triangular wave from Figure 10.2 is 2.
Periodic functions under scaling If 푓(푡) is periodic of period 푝and 푎is any positive number let 푔(푡) = 푓(푎푡).
Then for all 푡 푔 ( 푡+ 푝 푎 ) = 푓 ( 푎 ( 푡+ 푝 푎 )) = 푓(푎푡+ 푝) = 푓(푎푡) = 푔(푡).
Thus If 푓(푡) is periodic with period 푝, then 푓(푎푡) is periodic with period 푝 푎.
It is also true that if 푃is the fundamental period for the periodic function 푓(푡), then the fundamental period of 푔(푡) = 푓(푎푡) is 푃/푎. To see this it is only necessary to verify that any period 푟of 푔(푡) is at least as large as 푃/푎, which is already a period as observed above. But if 푟is a period for 푔(푡), then 푟푎is a period for 푔(푡/푎) = 푓(푡) so that 푟푎≥푃, or 푟≥푃/푎.
726 10 Fourier Series Applying these observations to the functions sin 푡and cos 푡with funda-mental period 2휋gives the following facts.
Theorem 1. For any 푎> 0 the functions cos 푎푡and sin 푎푡are periodic with period 2휋/푎. In particular, if 퐿> 0 then the functions cos 푛휋 퐿푡 and sin 푛휋 퐿푡, 푛= 1, 2, 3, . . . .
are periodic with fundamental period 푃= 2퐿/푛.
Note that since the fundamental period of the functions cos 푛휋 퐿푡and sin 푛휋 퐿푡 is 푃= 2퐿/푛, it follows that 2퐿= 푛푃is also a period for each of these functions. Thus, a sum ∞ ∑ 푛=1 ( 푎푛cos 푛휋 퐿푡+ 푏푛sin 푛휋 퐿푡 ) will be periodic of period 2퐿.
Notice that if 푛is a positive integer, then cos 푛푡and sin 푛푡are periodic with period 2휋/푛. Thus, each period of cos 푡or sin 푡contains 푛periods of cos 푛푡and sin 푛푡. This means that the functions cos 푛푡and sin 푛푡oscillate more rapidly as 푛increases, as can be seen in Figure 10.3 for 푛= 3.
1 −1 휋 −휋 (a) The graphs of cos 푡and cos 3푡.
1 −1 휋 −휋 (b) The graphs of sin 푡and sin 3푡.
Fig. 10.3 Example 2. Find the fundamental period of each of the following periodic functions.
1. cos 2푡 2. sin 3 2(푡−휋) 3. 1 + cos 푡+ cos 2푡 4. sin 2휋푡+ sin 3휋푡 ▶Solution.
1. 푃= 2휋/2 = 휋.
2. sin 3 2(푡−휋) = sin( 3 2푡−3 2휋) = sin 3 2푡cos 3 2휋−cos 3 2푡sin 3 2휋= cos 3 2푡. Thus, 푃= 2휋/(3/2) = 4휋/3.
10.1 Periodic Functions and Orthogonality Relations 727 3. The constant function 1 is periodic with any period 푝, the fundamental period of cos 푡is 2휋and all the periods are of the form 2푛휋for a positive integer 푛, and the fundamental period of cos 2푡is 휋with 푚휋being all the possible periods. Thus, the smallest number that works as a period for all the functions is 2휋and this is also the smallest period for the sum.
Hence 푃= 2휋.
4. The fundamental period of sin 2휋푡is 2휋/2휋= 1 so that all of the periods have the form 푛for 푛a positive integer, and the fundamental period of sin 3휋푡is 2휋/3휋= 2/3 so that all of the periods have the form 2푚/3 for 푚a positive integer. Thus, the smallest number that works as a period for both functions is 2 and thus 푃= 2.
◀ Orthogonality Relations for Sine and Cosine The family of linearly independent functions { 1, cos 휋 퐿푡, cos 2휋 퐿푡, cos 3휋 퐿푡, . . . , sin 휋 퐿푡, sin 2휋 퐿푡, sin 3휋 퐿푡, . . .
} form what is called a mutually orthogonal set of functions on the interval [−퐿, 퐿], analogous to a mutually perpendicular set of vectors. Two functions 푓and 푔defined on an interval 푎≤푡≤푏are said to be orthogonal on the interval [푎, 푏] if ∫푏 푎 푓(푡)푔(푡) 푑푡= 0.
A family of functions is mutually orthogonal on the interval [푎, 푏] if any two distinct functions are orthogonal. The mutual orthogonality of the family of cosine and sine functions on the interval [−퐿, 퐿] is a consequence of the following identities.
Proposition 3 (Orthogonality Relations). Let 푚and 푛be positive in-tegers, and let 퐿> 0. Then ∫퐿 −퐿 cos 푛휋 퐿푡푑푡= ∫퐿 −퐿 sin 푛휋 퐿푡푑푡= 0 (1) ∫퐿 −퐿 cos 푛휋 퐿푡sin 푚휋 퐿푡푑푡= 0 (2) ∫퐿 −퐿 cos 푛휋 퐿푡cos 푚휋 퐿푡푑푡= { 퐿, if 푛= 푚, 0 if 푛∕= 푚.
(3) ∫퐿 −퐿 sin 푛휋 퐿푡sin 푚휋 퐿푡푑푡= { 퐿, if 푛= 푚, 0 if 푛∕= 푚.
(4) 728 10 Fourier Series Proof. For (1): ∫퐿 −퐿 cos 푛휋 퐿푡푑푡= 퐿 푛휋sin 푛휋 퐿푡 퐿 −퐿 = 퐿 푛휋(sin 푛휋−sin(−푛휋)) = 0.
For (3) with 푛∕= 푚, use the identity cos 퐴cos 퐵= 1 2(cos(퐴+ 퐵) + cos(퐴−퐵)), to get ∫퐿 −퐿 cos 푛휋 퐿푡cos 푚휋 퐿푡푑푡= ∫퐿 −퐿 1 2 ( cos (푛+ 푚)휋 퐿 푡+ cos (푛−푚)휋 퐿 푡 ) 푑푡 = ( 퐿 2(푛+ 푚)휋sin (푛+ 푚)휋 퐿 푡+ 퐿 2(푛−푚)휋sin (푛−푚)휋 퐿 푡 ) 퐿 −퐿 = 0.
For (3) with 푛= 푚, use the identity cos2 퐴= (1 + cos 2퐴)/2 to get ∫퐿 −퐿 cos 푛휋 퐿푡cos 푚휋 퐿푡푑푡= ∫퐿 −퐿 ( cos 푛휋 퐿푡 )2 푑푡= = ∫퐿 −퐿 1 2 ( 1 + cos 2푛휋 퐿푡 ) 푑푡= 1 2 ( 푡+ 퐿 2푛휋sin 2푛휋 퐿푡 ) 퐿 −퐿 = 퐿.
The proof of (4) is similar, making use of the identities sin2 퐴= (1−cos 2퐴)/2 in case 푛= 푚and sin 퐴sin 퐵= 1 2(cos(퐴−퐵) −cos(퐴+ 퐵)) in case 푛∕= 푚. The proof of (2) is left as an exercise.
Even and Odd Functions A function 푓defined on a symmetric interval [−퐿, 퐿] is even if 푓(−푡) = 푓(푡) for −퐿≤푡≤퐿, and 푓is odd if 푓(−푡) = −푓(푡) for −퐿≤푡≤퐿.
Example 4. Determine whether each of the following functions is even, odd, or neither.
1. 푓(푡) = 3푡2 + cos 5푡 2. 푔(푡) = 3푡−푡2 sin 2푡 3. ℎ(푡) = 푡2 + 푡+ 1 ▶Solution.
1. Since 푓(−푡) = 3(−푡)2 + cos 5(−푡) = 3푡2 + cos 5푡= 푓(푡) for all 푡, it follows that 푓is an even function.
10.1 Periodic Functions and Orthogonality Relations 729 2. Since 푔(−푡) = 3(−푡) −(−푡)2 sin 3(−푡) = −3푡+ 푡2 sin 3푡= −푔(푡) for all 푡, it follows that 푔is an odd function.
3. Since ℎ(−푡) = (−푡)2 + (−푡) + 1 = 푡2 −푡+ 1 = 푡2 + 푡+ 1 = ℎ(푡) ⇐ ⇒ −푡= 푡⇐ ⇒푡= 0, we conclude that ℎis not even. Similarly, ℎ(−푡) = −ℎ(푡) ⇐ ⇒푡2−푡+1 = −푡2−푡−1 ⇐ ⇒푡2+1 = (−푡2+1) ⇐ ⇒푡2+1 = 0, which is not true for any 푡. Thus ℎis not odd, and hence it is neither even or odd.
◀ The graph of an even function is symmetric with respect to the 푦-axis, while the graph of an odd function is symmetric with respect to the origin, as illustrated in Figure 10.4.
푡 −푡 푓(푡) 푓(−푡) (a) The graph of an even function.
푡 −푡 푓(푡) 푓(−푡) = −푓(푡) (b) The graph of an odd function.
Fig. 10.4 Here is a list of basic properties of even and odd functions that are useful in applications to Fourier series. All of them follow easily from the definitions, and the verifications will be left to the exercises.
Proposition 5. Suppose that 푓and 푔are functions defined on the interval −퐿≤푡≤퐿.
1. If both 푓and 푔are even then 푓+ 푔and 푓푔are even.
2. If both 푓and 푔are odd, then 푓+ 푔is odd and 푓푔is even.
3. If 푓is even and 푔is odd, then 푓푔is odd.
4. If 푓is even, then ∫퐿 −퐿 푓(푡) 푑푡= 2 ∫퐿 0 푓(푡) 푑푡.
5. If 푓is odd, then ∫퐿 −퐿 푓(푡) 푑푡= 0.
Since the integral of 푓computes the signed area under the graph of 푓, the integral equations can be seen from the graphs of even and odd functions in Figure 10.4.
730 10 Fourier Series Exercises 1–9. Graph each of the following periodic functions. Graph at least 3 periods.
1. 푓(푡) = { 3 if 0 < 푡< 3 −3 if −3 < 푡< 0 ; 푓(푡+ 6) = 푓(푡).
2. 푓(푡) = ⎧ ⎨ ⎩ −3 if −2 ≤푡< −1 0 if −1 ≤푡≤1 3 if 1 < 푡< 2 ; 푓(푡+ 4) = 푓(푡).
3. 푓(푡) = 푡, 0 < 푡≤2; 푓(푡+ 2) = 푓(푡).
4. 푓(푡) = 푡, −1 < 푡≤1; 푓(푡+ 2) = 푓(푡).
5. 푓(푡) = sin 푡, 0 < 푡≤휋; 푓(푡+ 휋) = 푓(푡).
6. 푓(푡) = { 0 if −휋≤푡< 0 sin 푡 if 0 < 푡≤휋 ; 푓(푡+ 2휋) = 푓(푡).
7. 푓(푡) = { −푡 if −1 ≤푡< 0 1 if 0 ≤푡< 1 ; 푓(푡+ 2) = 푓(푡).
8. 푓(푡) = 푡2, −1 < 푡≤1; 푓(푡+ 2) = 푓(푡).
9. 푓(푡) = 푡2, 0 < 푡≤2; 푓(푡+ 2) = 푓(푡).
10–17. Determine if the given function is periodic. If it is periodic find the fundamental period.
10. 1 11. sin 2푡 12. 1 + cos 3휋푡 13. cos 2푡+ sin 3푡 14. 푡+ sin 2푡 15. sin2 푡 16. cos 푡+ cos 휋푡 17. sin 푡+ sin 2푡+ sin 3푡 18–26. Determine if the given function is even, odd, or neither.
10.2 Fourier Series 731 18. 푓(푡) = ∣푡∣ 19. 푓(푡) = 푡∣푡∣ 20. 푓(푡) = sin2 푡 21. 푓(푡) = cos2 푡 22. 푓(푡) = sin 푡sin 3푡 23. 푓(푡) = 푡2 + sin 푡 24. 푓(푡) = 푡+ ∣푡∣ 25. 푓(푡) = ln ∣cos 푡∣ 26. 푓(푡) = 5푡+ 푡2 sin 3푡 27. Verify the orthogonality property (2) from Proposition 3: ∫퐿 −퐿 cos 푛휋 퐿푡sin 푚휋 퐿푡푑푡= 0 28. Use the properties of even and odd functions (Proposition 10.4) to eval-uate the following integrals.
(a) ∫1 −1 푡푑푡 (b) ∫1 −1 푡4 푑푡 (c) ∫휋 −휋 푡sin 푡푑푡 (d) ∫휋 −휋 푡cos 푡푑푡 (e) ∫휋 −휋 cos 푛휋 퐿푡sin 푚휋 퐿푡푑푡 (f) ∫휋 −휋 푡2 sin 푡푑푡 10.2 Fourier Series We start by considering the possibility of representing a function 푓as a sum of a series of the form 푓(푡) = 푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) (1) 732 10 Fourier Series where the coefficients 푎0, 푎1, . . ., 푏1, 푏2, . . ., are to be determined. Since the individual terms in the series (1) are periodic with periods 2퐿, 2퐿/2, 2퐿/3, . . ., the function 푓(푡) determined by the sum of the series, where it converges, must be periodic with period 2퐿. This means that only periodic functions of period 2퐿can be represented by a series of the form (1). Our first problem is to find the coefficients 푎푛and 푏푛in the series (1). The first term of the series is written 푎0/2, rather than simply as 푎0, to make the formula to be derived below the same for all 푎푛, rather than a special case for 푎0.
The coefficients 푎푛and 푏푛can be found from the orthogonality relations of the family of functions cos(푛휋푡/퐿) and sin(푛휋푡/퐿) on the interval [−퐿, 퐿] given in Proposition 3 of Sect. 10.1. To compute the coefficient 푎푛for 푛= 1, 2, 3, . . ., multiply both sides of the series (1) by cos(푚휋푡/퐿), with 푚a positive integer and then integrate from −퐿to 퐿. For the moment we will assume that the integrals exist and that it is justified to integrate term by term. Then using (1), (2), and (3) from Sect. 10.1, we get ∫퐿 −퐿 푓(푡) cos 푚휋 퐿푡푑푡= 푎0 2 ∫퐿 −퐿 cos 푚휋 퐿푡푑푡 | {z } = 0 + ∞ ∑ 푛=1 [ 푎푛 ∫퐿 −퐿 cos 푛휋 퐿푡cos 푚휋 퐿푡푑푡 | {z } = ⎧ ⎨ ⎩ 0 if 푛∕= 푚 퐿 if 푛= 푚 +푏푛 ∫퐿 −퐿 sin 푛휋 퐿푡cos 푚휋 퐿푡푑푡 | {z } = 0 ] = 푎푚퐿.
Thus, 푎푚= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푚휋 퐿푡푑푡, 푚= 1, 2, 3, . . .
or, replacing the index 푚by 푛, 푎푛= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋 퐿푡푑푡, 푛= 1, 2, 3, . . .
(2) To compute 푎0, integrate both sides of (1) from −퐿to 퐿to get ∫퐿 −퐿 푓(푡) 푑푡= 푎0 2 ∫퐿 −퐿 푑푡 | {z } =2퐿 + ∞ ∑ 푛=1 [ 푎푛 ∫퐿 −퐿 cos 푛휋 퐿푡푑푡 | {z } =0 +푏푛 ∫퐿 −퐿 sin 푛휋 퐿푡푑푡 | {z } = 0 ] = 푎0퐿.
Thus, 푎0 = 1 퐿 ∫퐿 −퐿 푓(푡) 푑푡.
(3) 10.2 Fourier Series 733 Hence, 푎0 is two times the average value of the function 푓(푡) over the interval −퐿≤푡≤퐿. Observe that the value of 푎0 is obtained from (2) by setting 푛= 0. Of course, if the constant 푎0 in (1) were not divided by 2, we would need a separate formula for 푎0. It is for this reason that the constant term in (1) is labeled 푎0/2. Thus, for all 푛≥0, the coefficients 푎푛are given by a single formula 푎푛= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋 퐿푡푑푡, 푛= 0, 1, 2, . . .
(4) To compute 푏푛for 푛= 1, 2, 3, . . ., multiply both sides of the series (1) by sin(푚휋푡/퐿), with 푚a positive integer and then integrate from −퐿to 퐿.
Then using (1), (2), and (4) from Sect. 10.1, we get ∫퐿 −퐿 푓(푡) sin 푚휋 퐿푡푑푡= 푎0 2 ∫퐿 −퐿 sin 푚휋 퐿푡푑푡 | {z } = 0 + ∞ ∑ 푛=1 [ 푎푛 ∫퐿 −퐿 cos 푛휋 퐿푡sin 푚휋 퐿푡푑푡 | {z } = 0 +푏푛 ∫퐿 −퐿 sin 푛휋 퐿푡sin 푚휋 퐿푡푑푡 | {z } = ⎧ ⎨ ⎩ 0 if 푛∕= 푚 퐿 if 푛= 푚 ] = 푏푚퐿.
Thus, replacing the index 푚by 푛, we find that 푏푛= 1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋 퐿푡푑푡, 푛= 1, 2, 3, . . .
(5) We have arrived at what are known as the Euler Formulas for a function 푓(푡) that is the sum of a trigonometric series as in (1): 푎0 = 1 퐿 ∫퐿 −퐿 푓(푡) 푑푡 (6) 푎푛= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋 퐿푡푑푡, 푛= 1, 2, 3, . . .
(7) 푏푛= 1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋 퐿푡푑푡, 푛= 1, 2, 3, . . .
(8) The numbers 푎푛and 푏푛are known as the Fourier coefficients of the func-tion 푓. Note that while we started with a periodic function of period 2퐿, the formulas for 푎푛and 푏푛only use the values of 푓(푡) on the interval [−퐿, 퐿].
734 10 Fourier Series We can then reverse the process, and start with any function 푓(푡) defined on the symmetric interval [−퐿, 퐿] and use the Euler formulas to determine a trigonometric series. We will write 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) , (9) where the 푎푛, 푏푛are defined by (6), (7), and (8), to indicate that the right hand side of (9) is the Fourier series of the function 푓(푡) defined on [−퐿, 퐿].
Note that the symbol ∼indicates that the trigonometric series on the right of (9) is associated with the function 푓(푡); it does not imply that the series converges to 푓(푡) for any value of 푡. In fact, there are functions whose Fourier series do not converge to the function. Of course, we will be interested in the conditions under which the Fourier series of 푓(푡) converges to 푓(푡), in which case ∼can be replaced by =; but for now we associate a specific series using Equations (6), (7), and (8) with 푓(푡) and call it the Fourier series. The mild conditions under which the Fourier series of 푓(푡) converges to 푓(푡) will be considered in the next section.
Remark 1. If an integrable function 푓(푡) is periodic with period 푝, then the integral of 푓(푡) over any interval of length 푝is the same; that is ∫푐+푝 푐 푓(푡) 푑푡= ∫푝 0 푓(푡) 푑푡 (10) for any choice of 푐. To see this, first observe that for any 훼and 훽, if we use the change of variables 푡= 푥−푝, then ∫훽 훼 푓(푡) 푑푡= ∫훽+푝 훼+푝 푓(푥−푝) 푑푥= ∫훽+푝 훼+푝 푓(푥) 푑푥= ∫훽+푝 훼+푝 푓(푡) 푑푡.
Letting 훼= 푐and 훽= 0 gives ∫0 푐 푓(푡) 푑푡= ∫푝 푐+푝 푓(푡) 푑푡 so that ∫푐+푝 푐 푓(푡) 푑푡= ∫0 푐 푓(푡) 푑푡+ ∫푐+푝 0 푓(푡) 푑푡 = ∫푝 푐+푝 푓(푡) 푑푡+ ∫푐+푝 0 푓(푡) 푑푡= ∫푝 0 푓(푡) 푑푡, which is (10). This formula means that when computing the Fourier coeffi-cients, the integrals can be computed over any convenient interval of length 2퐿. For example, 10.2 Fourier Series 735 푎푛= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋 퐿푡푑푡= 1 퐿 ∫2퐿 0 푓(푡) cos 푛휋 퐿푡푑푡.
We now consider some examples of the calculation of Fourier series.
Example 2. Compute the Fourier series of the odd square wave function of period 2퐿and amplitude 1 given by 푓(푡) = { −1 −퐿≤푡< 0, 1 0 ≤푡< 퐿, ; 푓(푡+ 2퐿) = 푓(푡).
See Figure 10.5 for the graph of 푓(푡).
푦 푡 1 −1 퐿 2퐿 3퐿 −퐿 −2퐿 −3퐿 Fig. 10.5 The odd square wave of period 2퐿 ▶Solution. Use the Euler formulas for 푎푛(Equations (6) and (7)) to con-clude 푎푛= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋 퐿푡푑푡= 0 for all 푛≥0. This is because the function 푓(푡) cos 푛휋 퐿푡is the product of an odd and even function, and hence is odd, which implies by Proposition 5 (Part 5) of Section 10.1 that the integral is 0. It remains to compute the coefficients 푏푛from (8).
푏푛= 1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋 퐿푡푑푡= 1 퐿 ∫0 −퐿 푓(푡) sin 푛휋 퐿푡푑푡+ 1 퐿 ∫퐿 0 푓(푡) sin 푛휋 퐿푡푑푡 = 1 퐿 ∫0 −퐿 (−1) sin 푛휋 퐿푡푑푡+ 1 퐿 ∫퐿 0 (+1) sin 푛휋 퐿푡푑푡 = 1 퐿 {[ 퐿 푛휋cos 푛휋 퐿푡 ]0 −퐿 − [ 퐿 푛휋cos 푛휋 퐿푡 ]퐿 0 } = 1 푛휋[(1 −cos(−푛휋)) + (1 −cos(푛휋))] = 2 푛휋(1 −cos 푛휋) = 2 푛휋(1 −(−1)푛).
Therefore, 736 10 Fourier Series 푏푛= { 0 if 푛is even, 4 푛휋 if 푛is odd, and the Fourier series is 푓(푡) ∼4 휋 ( sin 휋 퐿푡+ 1 3 sin 3휋 퐿푡+ 1 5 sin 5휋 퐿푡+ 1 7 sin 7휋 퐿푡+ ⋅⋅⋅ ) .
(11) ◀ Example 3. Compute the Fourier series of the even square wave function of period 2퐿and amplitude 1 given by 푓(푡) = ⎧ ⎨ ⎩ −1 −퐿≤푡< −퐿/2, 1 −퐿/2 ≤푡< 퐿/2, −1 퐿/2 ≤푡< 퐿, ; 푓(푡+ 2퐿) = 푓(푡).
See Figure 10.6 for the graph of 푓(푡).
푦 푡 1 −1 퐿 2 3퐿 2 5퐿 2 −퐿 2 −3퐿 2 −5퐿 2 Fig. 10.6 The even square wave of period 2퐿 ▶Solution. Use the Euler formulas for 푏푛(Equation (8)) to conclude 푏푛= 1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋 퐿푡푑푡= 0, for all 푛≥1. As in the previous example, this is because the function 푓(푡) sin 푛휋 퐿푡is the product of an even and odd function, and hence is odd, which implies by Proposition 5 (Part 5) of Section 10.1 that the integral is 0. It remains to compute the coefficients 푎푛from (6) and (7).
For 푛= 0, 푎0 is twice the average of 푓(푡) over the period [−퐿, 퐿], which is easily seen to be 0 from the graph of 푓(푡). For 푛≥1, 푎푛= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋 퐿푡푑푡 = 1 퐿 ∫−퐿/2 −퐿 푓(푡) cos 푛휋 퐿푡푑푡+ 1 퐿 ∫퐿/2 −퐿/2 푓(푡) cos 푛휋 퐿푡푑푡+ 1 퐿 ∫퐿 퐿/2 푓(푡) cos 푛휋 퐿푡푑푡 10.2 Fourier Series 737 = 1 퐿 ∫−퐿/2 −퐿 (−1) cos 푛휋 퐿푡푑푡+ 1 퐿 ∫퐿/2 −퐿/2 (+1) cos 푛휋 퐿푡푑푡+ 1 퐿 ∫퐿 퐿/2 (−1) cos 푛휋 퐿푡푑푡 = 1 퐿 { − [ 퐿 푛휋sin 푛휋 퐿푡 ]−퐿/2 −퐿 + [ 퐿 푛휋sin 푛휋 퐿푡 ]퐿/2 −퐿/2 − [ 퐿 푛휋sin 푛휋 퐿푡 ]퐿 퐿/2 } = 1 푛휋 [ −sin ( −푛휋 2 ) + sin(−푛휋) + sin (푛휋 2 ) −sin ( −푛휋 2 ) −sin 푛휋+ sin (푛휋 2 )] = 4 푛휋sin 푛휋 2 .
Therefore, 푎푛= ⎧ ⎨ ⎩ 0 if 푛is even, 4 푛휋 if 푛= 4푚+ 1 −4 푛휋 if 푛= 4푚+ 3 and the Fourier series is 푓(푡) ∼4 휋 ( cos 휋 퐿푡−1 3 cos 3휋 퐿푡+ 1 5 cos 5휋 퐿푡−1 7 cos 7휋 퐿푡+ ⋅⋅⋅ ) = 4 휋 ∞ ∑ 푘=0 (−1)푘 2푘+ 1 cos (2푘+ 1)휋 퐿 푡.
◀ Example 4. Compute the Fourier series of the even triangular wave func-tion of period 2휋given by 푓(푡) = { −푡 −휋≤푡< 0, 푡 0 ≤푡< 휋, ; 푓(푡+ 2휋) = 푓(푡).
See Figure 10.7 for the graph of 푓(푡).
휋 2휋 3휋 −휋 −2휋 −3휋 0 휋 Fig. 10.7 The even triangular wave of period 2휋.
▶Solution. The period is 2휋= 2퐿so 퐿= 휋. Again, since the function 푓(푡) is even, the coefficients 푏푛= 0. It remains to compute the coefficients 푎푛 from the Euler formulas (6) and (7).
For 푛= 0, using the fact that 푓(푡) is even, 738 10 Fourier Series 푎0 = 1 휋 ∫휋 −휋 푓(푡) 푑푡= 2 휋 ∫휋 0 푓(푡) 푑푡 = 2 휋 ∫휋 0 푡푑푡= 2 휋 푡2 2 휋 0 = 휋.
For 푛≥1, using the fact that 푓(푡) is even, and taking advantage of the integration by parts formula ∫ 푥cos 푥푑푥= 푥sin 푥+ cos 푥+ 퐶, 푎푛= 1 휋 ∫휋 −휋 푓(푡) cos 푛푡푑푡= 2 휋 ∫휋 0 푓(푡) cos 푛푡푑푡 = 2 휋 ∫휋 0 푡cos 푛푡푑푡 ( let 푥= 푛푡so 푡= 푥 푛and 푑푡= 푑푥 푛 ) = 2 휋 ∫푛휋 0 푥 푛cos 푥푑푥 푛= 2 푛2휋[푥sin 푥+ cos 푥]푥=푛휋 푥=0 = 2 푛2휋[cos 푛휋−1] = 2 푛2휋[(−1)푛−1] Therefore, 푎푛= { 0 if 푛is even, − 4 푛2휋 if 푛is odd and the Fourier series is 푓(푡) ∼휋 2 −4 휋 (cos 푡 12 + cos 3푡 32 + cos 5푡 52 + cos 7푡 72 + ⋅⋅⋅ ) = 휋 2 −4 휋 ∞ ∑ 푘=0 cos(2푘+ 1)푡 (2푘+ 1)2 .
◀ Example 5. Compute the Fourier series of the sawtooth wave function of period 2퐿given by 푓(푡) = 푡 for −퐿≤푡< 퐿; 푓(푡+ 2퐿) = 푓(푡).
See Figure 10.8 for the graph of 푓(푡).
▶Solution. As in Example 2, the function 푓(푡) is odd, so the cosine terms 푎푛are all 0. Now compute the coefficients 푏푛from (8). Using the integration by parts formula 10.2 Fourier Series 739 푦 푡 퐿 −퐿 퐿 2퐿 3퐿 −퐿 −2퐿 −3퐿 Fig. 10.8 The sawtooth wave of period 2퐿 ∫ 푥sin 푥푑푥= sin 푥−푥cos 푥+ 퐶, 푏푛= 1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋 퐿푡푑푡 = 2 퐿 ∫퐿 0 푡sin 푛휋 퐿푡푑푡 ( let 푥= 푛휋 퐿푡so 푡= 퐿 푛휋푥and 푑푡= 퐿 푛휋푑푥 ) = 2 퐿 ∫푛휋 0 퐿 푛휋푥sin 푥퐿푑푥 푛휋 = 2퐿 푛2휋2 ∫푛휋 0 푥sin 푥푑푥 = 2퐿 푛2휋2 [sin 푥−푥cos 푥]푥=푛휋 푥=0 = −2퐿 푛2휋2 (푛휋cos 푛휋) = −2퐿 푛휋(−1)푛.
Therefore, the Fourier series is 푓(푡) ∼2퐿 휋 ( sin 휋 퐿푡−1 2 sin 2휋 퐿푡+ 1 3 sin 3휋 퐿푡−1 4 sin 4휋 퐿푡+ ⋅⋅⋅ ) = 2퐿 휋 ∞ ∑ 푛=1 (−1)푛+1 푛 sin 푛휋 퐿푡.
◀ All of the examples so far have been of functions that are either even or odd. If a function 푓(푡) is even, the resulting Fourier series will only have cosine terms, as in the case of Examples 3 and 4, while if 푓(푡) is odd, the resulting Fourier series will only have sine terms, as in Examples 2 and 5.
Here are some examples where both sine an cosine terms appear.
Example 6. Compute the Fourier series of the function of period 4 given by 740 10 Fourier Series 푓(푡) = { 0 −2 ≤푡< 0, 푡 0 ≤푡< 2, ; 푓(푡+ 4) = 푓(푡).
See Figure 10.9 for the graph of 푓(푡).
2 2 4 6 −2 −4 −6 푦 푡 Fig. 10.9 A half sawtooth wave of period 4 ▶Solution. This function is neither even nor odd, so we expect both sine and cosine terms to be present. The period is 4 = 2퐿so 퐿= 2. Because 푓(푡) = 0 on the interval (−2, 0), each of the integrals in the Euler formulas, which should be an integral from 푡= −2 to 푡= 2, can be replaced with an integral from 푡= 0 to 푡= 2. Thus, the Euler formulas give 푎0 = 1 2 ∫2 0 푡푑푡= 1 2 [푡2 2 ]2 0 = 1; 푎푛= 1 2 ∫2 0 푡cos 푛휋 2 푡푑푡 ( let 푥= 푛휋 2 푡so 푡= 2푥 푛휋and 푑푡= 2푑푥 푛휋 ) = 1 2 ∫푛휋 0 2푥 푛휋cos 푥2푑푥 푛휋= 2 푛2휋2 ∫푛휋 0 푥cos 푥푑푥 = 2 푛2휋2 [cos 푥+ 푥sin 푥]푥=푛휋 푥=0 = 2 푛2휋2 (cos 푛휋−1) = 2 푛2휋2 ((−1)푛−1).
Therefore, 푎푛= ⎧ ⎨ ⎩ 1 if 푛= 0, 0 if 푛is even and 푛≥2, − 4 푛2휋2 if 푛is odd.
Now compute 푏푛: 푏푛= 1 2 ∫2 0 푡sin 푛휋 2 푡푑푡 ( let 푥= 푛휋 2 푡so 푡= 2푥 푛휋and 푑푡= 2푑푥 푛휋 ) 10.2 Fourier Series 741 = 1 2 ∫푛휋 0 2푥 푛휋sin 푥2푑푥 푛휋= 2 푛2휋2 ∫푛휋 0 푥sin 푥푑푥 = 2 푛2휋2 [sin 푥−푥cos 푥]푥=푛휋 푥=0 = 2 푛2휋2 (−푛휋cos 푛휋) = −2 푛휋(−1)푛.
Thus, 푏푛= 2(−1)푛+1 푛휋 for all 푛≥1.
Therefore, the Fourier series is 푓(푡) ∼1 2 −4 휋2 ∞ ∑ 푘=0 1 (2푘+ 1)2 cos (2푘+ 1)휋 2 푡+ 2 휋 ∞ ∑ 푛=1 (−1)푛+1 푛 sin 푛휋 2 푡.
◀ Example 7. Compute the Fourier series of the square pulse wave function of period 2휋given by 푓(푡) = { 1 0 ≤푡< ℎ, 0 ℎ≤푡< 2휋, ; 푓(푡+ 2휋) = 푓(푡).
See Figure 10.10 for the graph of 푓(푡).
0 1 ℎ 2휋 −2휋 4휋 −4휋 Fig. 10.10 A square pulse wave of period 2휋.
▶Solution. For this function, it is more convenient to compute the 푎푛and 푏푛using integration over the interval [0, 2휋] rather than the interval [−휋, 휋].
Thus, 푎0 = 1 휋 ∫2휋 0 푓(푡) 푑푡= 1 휋 ∫ℎ 0 1 푑푡= ℎ 휋, 푎푛= 1 휋 ∫ℎ 0 cos 푛푡푑푡= sin 푛ℎ 휋푛 , and 푏푛= 1 휋 ∫ℎ 0 sin 푛푡푑푡= 1 −cos 푛ℎ 휋푛 , 742 10 Fourier Series and the Fourier series is 푓(푡) ∼ℎ 2휋+ 1 휋 ∞ ∑ 푛=1 (sin 푛ℎ 푛 cos 푛푡+ 1 −cos 푛ℎ 푛 sin 푛푡 ) .
◀ If the square pulse wave 푓(푡) is divided by ℎ, then one obtains a function whose graph is a series of tall thin rectangles of height 1/ℎand base ℎ, so that each of the rectangles with the bases starting at 2푛휋has area 1, as in Figure 10.11. Now consider the limiting case where ℎapproaches 0. The 0 1 ℎ ℎ 2휋 −2휋 4휋 −4휋 Fig. 10.11 A square unit pulse wave of period 2휋.
graph becomes a series of infinite height spikes of width 0 as in Figure 10.12.
This looks like an infinite sum of Dirac delta functions, which is the regular delta function extended to be periodic of period 2휋. That is, lim ℎ→0 푓(푡) ℎ = ∞ ∑ 푛=−∞ 훿(푡−2푛휋).
Now compute the Fourier coefficients 푎푛/ℎand 푏푛/ℎas ℎapproaches 0.
푎푛= sin 푛ℎ 휋푛ℎ→1 휋 and 푏푛= 1 −cos 푛ℎ 휋푛ℎ →0 as ℎ→0 Also, 푎0/ℎ= 1/휋. Thus, the 2휋-periodic delta function has a Fourier series ∞ ∑ 푛=−∞ 훿(푡−2푛휋) ∼1 2휋+ 1 휋 ∞ ∑ 푛=1 cos 푛푡.
(12) It is worth pointing out that this is one series that definitely does not converge for all 푡. In fact it does not converge for 푡= 0. However, there is a sense of convergence in which convergence makes sense. We will discuss this in the next section.
10.2 Fourier Series 743 0 2휋 −2휋 4휋 −4휋 Fig. 10.12 The limiting square unit pulse wave of period 2휋as ℎ→0.
Example 8. Compute the Fourier series of the function 푓(푡) = sin 2푡+ 5 cos3푡.
▶Solution. Since 푓(푡) is periodic of period 2휋and is already given as a sum of sines and cosines, no further work is needed. The coefficients can be read offwithout any integration as 푎푛= 0 for 푛∕= 3 and 푎3 = 5 while 푏푛= 0 for 푛∕= 2 and 푏2 = 1. The same results would be obtained by integration using Euler’s formulas.
Example 9. Compute the Fourier series of the function 푓(푡) = sin3 푡 ▶Solution. This can be handled by trig identities to reduce it to a finite sum of terms of the form sin 푛푡.
sin3 푡= sin 푡sin2 푡= 1 2 sin 푡(1 −cos 2푡) = 1 2 sin 푡−1 2 sin 푡cos 2푡= 1 2 sin 푡−1 2 (1 2(sin 3푡+ sin(−푡)) ) = 3 4 sin 푡−1 4 sin 3푡 The right hand side is the Fourier series of sin3 푡.
Exercises 1–17. Find the Fourier series of the given periodic function.
1. 푓(푡) = { 0 if −5 ≤푡< 0 3 if 0 ≤푡< 5 ; 푓(푡+ 10) = 푓(푡).
2. 푓(푡) = { 2 if −휋≤푡< 0 −2 if 0 ≤푡< 휋 ; 푓(푡+ 2휋) = 푓(푡).
744 10 Fourier Series 3. 푓(푡) = { 4 if −휋≤푡< 0 −1 if 0 ≤푡< 휋 ; 푓(푡+ 2휋) = 푓(푡).
4. 푓(푡) = 푡, 0 ≤푡< 2; 푓(푡+ 2) = 푓(푡).
Hint: It may be useful to take advantage of Equation (10) in applying the Euler formulas.
5. 푓(푡) = 푡, −휋≤푡< 휋; 푓(푡+ 2휋) = 푓(푡).
6. 푓(푡) = ⎧ ⎨ ⎩ 0 0 ≤푡< 1, 1 1 ≤푡< 2, 0 2 ≤푡< 3, 푓(푡+ 3) = 푓(푡).
7. 푓(푡) = 푡2, −2 ≤푡< 2; 푓(푡+ 4) = 푓(푡).
8. 푓(푡) = { 0 if −1 ≤푡< 0 푡2 if 0 ≤푡< 1 ; 푓(푡+ 2) = 푓(푡).
9. 푓(푡) = sin 푡, 0 ≤푡< 휋; 푓(푡+ 휋) = 푓(푡).
10. 푓(푡) = { 0 if −휋≤푡< 0 sin 푡 if 0 ≤푡< 휋 ; 푓(푡+ 2휋) = 푓(푡).
11. 푓(푡) = { 1 + 푡 if −1 ≤푡< 0 1 −푡 if 0 ≤푡< 1 ; 푓(푡+ 2) = 푓(푡).
12. 푓(푡) = { 1 + 푡 if −1 ≤푡< 0 −1 + 푡 if 0 ≤푡< 1 ; 푓(푡+ 2) = 푓(푡).
13. 푓(푡) = { −푡(휋+ 푡) if −휋≤푡< 0 푡(휋−푡) if 0 ≤푡< 휋 ; 푓(푡+ 2휋) = 푓(푡).
14. 푓(푡) = 3 cos2 푡, −휋≤푡< 휋; 푓(푡+ 2휋) = 푓(푡) 15. 푓(푡) = sin 푡 2, −휋≤푡< 휋; 푓(푡+ 2휋) = 푓(푡) 16. 푓(푡) = sin 푝푡, −휋≤푡< 휋; 푓(푡+ 2휋) = 푓(푡) (where 푝is not an integer) 17. 푓(푡) = 푒푡; −1 ≤푡< 1; 푓(푡+ 2) = 푓(푡) Then, 푎푛= ∫1 −1 푒푡cos 푛휋푡푑푡 10.3 Convergence of Fourier Series 745 = 1 1 + 푛2휋2 푒푡[cos 푛휋푡+ 푛휋sin 푛휋푡] 1 −1 = 1 1 + 푛2휋2 [푒1 cos 푛휋−푒−1 cos(−푛휋)] = (푒1 −푒−1)(−1)푛 1 + 푛2휋2 = 2(−1)푛sinh(1) 1 + 푛2휋2 , and, 푏푛= ∫1 −1 푒푡sin 푛휋푡푑푡 = 1 1 + 푛2휋2 푒푡[sin 푛휋푡−푛휋cos 푛휋푡] 1 −1 = 1 1 + 푛2휋2 [푒1(−푛휋cos 푛휋) −푒−1(−푛휋cos(−푛휋))] = (푒1 −푒−1)(−푛휋)(−1)푛 1 + 푛2휋2 = 2(−1)푛(−푛휋) sinh(1) 1 + 푛2휋2 .
Therefore, the Fourier series is 푓(푡) ∼sinh(1) + 2 sinh(1) ∞ ∑ 푛=1 (−1)푛(cos 푛휋푡−푛휋sin 푛휋푡) 1 + 푛2휋2 .
10.3 Convergence of Fourier Series If 푓(푡) is a periodic function of period 2퐿, the Fourier series of 푓(푡) is 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) , (1) where the coefficients 푎푛and 푏푛are given by the Euler formulas 푎푛= 1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋 퐿푡푑푡, 푛= 0, 1, 2, 3, . . .
(2) 푏푛= 1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋 퐿푡푑푡, 푛= 1, 2, 3, . . .
(3) The questions that we wish to consider are (1) under what conditions on the function 푓(푡) is it true that the series converges, and (2) when does it converge to the original function 푓(푡)?
As with any infinite series, to say that ∑∞ 푛=1 푐푛= 퐶means that the sequence of partial sums ∑푚 푛=1 푐푛= 푆푚converges to 퐶, that is, 746 10 Fourier Series lim 푚→∞푆푚= 퐶.
The partial sums of the Fourier series (1) are 푆푚(푡) = 푎0 2 + 푚 ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) .
(4) The partial sum 푆푚(푡) is a finite linear combination of the trigonometric functions cos 푛휋푡 퐿 and sin 푛휋푡 퐿, each of which is periodic of period 2퐿. Thus, 푆푚(푡) is also periodic of period 2퐿, and if the partial sums converge to a function 푔(푡), then 푔(푡) must also be periodic of period 2퐿.
Example 1. Consider the odd square wave function of period 2 and am-plitude 1 from Example 2 of Section 10.2 푓(푡) = { −1 −1 ≤푡< 0, 1 0 ≤푡< 1, ; 푓(푡+ 2) = 푓(푡).
(5) The Fourier series of this function was found to be (letting 퐿= 1) 푓(푡) ∼4 휋 ( sin 휋푡+ 1 3 sin 3휋푡+ 1 5 sin 5휋푡+ 1 7 sin 7휋푡+ ⋅⋅⋅ ) (6) = 4 휋 ∞ ∑ 푘=0 1 2푘+ 1 sin(2푘+ 1)휋푡.
Letting 푡= 0 in this series gives 4 휋 ∞ ∑ 푘=0 1 2푘+ 1 sin(2푘+ 1)휋0 = 4 휋 ∞ ∑ 푘=0 0 = 0.
Since 푓(0) = 1, it follows that the Fourier series does not converge to 푓(푡) for all 푡. Several partial sums 푆푚are graphed along with the graph of 푓(푡) in Figure 10.13. It can be seen that the graph of 푆15(푡) is very close to the graph of 푓(푡), except at the points of discontinuity, which are 0, ±1, ±2, . . .. This suggests that the Fourier series of 푓(푡) converges to 푓(푡) at all points except for where 푓(푡) has a discontinuity, which occurs whenever 푡is an integer 푛.
For each integer 푛, 푆푚(푛) = 4 휋 [ 푚 2 ] ∑ 푘=0 1 2푘+ 1 sin(2푘+ 1)휋푛= 4 휋 [ 푚 2 ] ∑ 푘=0 0 = 0.
Hence the Fourier series converges to 푓(푡) whenever 푡is not an integer and it converges to 0, which is the midpoint of the jump of 푓(푡) at each integer.
10.3 Convergence of Fourier Series 747 1 −1 1 2 3 −1 −2 −3 푦 푡 푆1(푡) = 4 휋sin 휋푡 1 −1 1 2 3 −1 −2 −3 푦 푡 푆5(푡) = 4 휋 ( sin 휋푡+ 1 3 sin 3휋푡+ 1 5 sin 5휋푡) 1 −1 1 2 3 −1 −2 −3 푦 푡 푆15(푡) = 4 휋 ∑7 푘=0 1 2푘+1 sin(2푘+ 1)휋푡 Fig. 10.13 Fourier series approximations 푆푚to the odd square wave of period 2 for 푚= 1, 5, and 15.
Similar results are true for a broad range of functions. We will describe the types of functions to which the convergence theorem applies and then state the convergence theorem.
Recall that a function 푓(푡) defined on an interval 퐼has a jump discon-tinuity at a point 푡= 푎if the left hand limit 푓(푎−) = lim푡→푎−푓(푡) and the right hand limit 푓(푎+) = lim푡→푎+ 푓(푡) both exist (as real numbers, not ±∞) and 푓(푎+) ∕= 푓(푎−).
748 10 Fourier Series The difference 푓(푎+) −푓(푎−) is frequently referred to as the jump in 푓(푡) at 푡= 푎. For example the odd square wave function of Example 10.2.2 has jump discontinuities at the points ±푛퐿for 푛= 0, 1, 2, . . . and the sawtooth wave function of Example 10.2.5 has jump discontinuities at ±푛for 푛= 0, 1, 2, . . .. On the other hand, the function 푔(푡) = tan 푡is a periodic function of period 휋that is discontinuous at the points 휋 2 + 푘휋for all integers 푘, but the discontinuity is not a jump discontinuity since, for example lim 푡→휋 2 −tan 푡= +∞, and lim 푡→휋 2 + tan 푡= −∞.
A function 푓(푡) is piecewise continuous on a closed interval [푎, 푏] if 푓(푡) is continuous except for possibly finitely many jump discontinuities in the in-terval [푎, 푏]. A function 푓(푡) is piecewise continuous for all 푡if it is piecewise continuous on every bounded interval. In particular, this means that there can be only finitely many discontinuities in any given bounded interval, and each of those must be a jump discontinuity. For convenience it will not be required that 푓(푡) be defined at the jump discontinuities, or 푓(푡) can be de-fined arbitrarily at the jump discontinuities. The square waves and sawtooth waves from Section 10.2 are typical examples of piecewise continuous periodic functions, while tan 푡is not piecewise continuous since the discontinuities are not jump discontinuities.
A function 푓(푡) is piecewise smooth if it is piecewise continuous and the derivative 푓′(푡) is also piecewise continuous. As with the convention on piecewise continuous, 푓′(푡) may not exist at finitely many points in any closed interval. All of the examples of periodic functions from Section 10.2 are piece-wise smooth. The property of 푓(푡) being piecewise smooth and periodic is sufficient to guarantee that the Fourier series of 푓(푡) converges, and the sum can be computed. This is the content of the following theorem.
Theorem 2. (Convergence of Fourier Series) Suppose that 푓(푡) is a periodic piecewise smooth function of period 2퐿. Then the Fourier series (1) converges (a) to the value 푓(푡) at each point 푡where 푓is continuous, and (b) to the value 1 2 [푓(푡+) + 푓(푡−)] at each point where 푓is not continuous.
Note that 1 2 [푓(푡+) + 푓(푡−)] is the average of the left-hand and right-hand limits of 푓at the point 푡. If 푓is continuous at 푡, then 푓(푡+) = 푓(푡) = 푓(푡−), so that 푓(푡) = 푓(푡+) + 푓(푡−) 2 , (7) for any 푡where 푓is continuous. Hence Theorem 2 can be rephrased as follows: The Fourier series of a piecewise smooth periodic function 푓converges for every 푡to the average of the left-hand and right-hand limits of 푓.
10.3 Convergence of Fourier Series 749 Example 3. Continuing with the odd square wave function of Example 1, it is clear from Equation (5) or from Figure 10.13 that if 푛is an even integer, then lim 푡→푛+ 푓(푡) = +1 and lim 푡→푛−푓(푡) = −1, while if 푛is an odd integer, then lim 푡→푛+ 푓(푡) = −1 and lim 푡→푛−푓(푡) = +1.
Therefore, whenever 푛is an integer, 푓(푛+) + 푓(푛−) 2 = 0.
This is consistent with Theorem 2 since the Fourier series (6) converges to 0 whenever 푡is an integer 푛(because sin(2푘+ 1)휋푛= 0).
For any point 푡other than an integer, the function 푓(푡) is continuous, so Theorem 2 gives an equality 푓(푡) = 4 휋 ( sin 휋푡+ 1 3 sin 3휋푡+ 1 5 sin 5휋푡+ 1 7 sin 7휋푡+ ⋅⋅⋅ ) .
By redefining 푓(푡) at integers to be 푓(푛) = 0 for integers 푛, then this equality holds for all 푡. Figure 10.14 shows the graph of the redefined function. Putting 1 −1 1 2 3 −1 −2 −3 푦 푡 Fig. 10.14 The odd square wave of period 2 redefined so that the Fourier series converges to 푓(푡) for all 푡.
in the value of 푓(푡) for some values of 푡leads to a trigonometric identity 4 휋 ( sin 휋푡+ 1 3 sin 3휋푡+ 1 5 sin 5휋푡+ 1 7 sin 7휋푡+ ⋅⋅⋅ ) = 푓(푡) = 1 if 0 < 푡< 1.
Letting 푡= 1/2 then gives the series 750 10 Fourier Series 1 −1 3 + 1 5 −1 7 + ⋅⋅⋅= 휋 4 .
Example 4. Let 푓be periodic of period 2 and defined on the interval 0 ≤ 푡< 2 by 푓(푡) = 푡2. Without computing the Fourier coefficients, give an explicit description of the sum of the Fourier series of 푓for all 푡.
▶Solution. The function is defined in only one period so the periodic extension is defined by 푓(푡) = 푡2 for 0 ≤푡< 2; 푓(푡+ 2) = 푓(푡).
Both 푓(푡) and 푓′(푡) are continuous everywhere except at the even integers.
Thus, the Fourier series converges to 푓(푡) everywhere except at the even integers. At the even integer 2푚the left and right limits are 푓(2푚−) = lim 푡→2푚−푓(푡) = lim 푡→0−푓(푡) = lim 푡→0−(푡+ 2)2 = 4, and 푓(2푚+) = lim 푡→2푚+ 푓(푡) = lim 푡→0+ 푓(푡) = lim 푡→0+ 푡2 = 0.
Therefore the sum of the Fourier series at 푡= 2푚is 푓(2푚−) + 푓(2푚+) 2 = 4 + 0 2 = 2.
The graph of the sum is shown in Figure 10.15.
◀ 4 2 4 6 −2 −4 −6 b b b b b b b 푦 푡 Fig. 10.15 The graph of sum of the Fourier series of the period 2 function 푓(푡) for Example 4.
Example 5. The 2휋-periodic delta function ∑∞ 푛=−∞훿(푡−2푛휋) has a Fourier series ∞ ∑ 푛=−∞ 훿(푡−2푛휋) ∼1 2휋+ 1 휋 ∞ ∑ 푛=1 cos 푛푡 (8) 10.3 Convergence of Fourier Series 751 that was computed in Section 10.2. See Figure 10.12 for the graph of ∑∞ 푛=−∞훿(푡−2푛휋). The 2휋-periodic delta function does not satisfy the con-ditions of the convergence theorem. Moreover, it is clear that the series does not converge since the individual terms do not approach 0. If 푡= 0 the series becomes 1 2휋+ 1 휋[1 + 1 + 1 + ⋅⋅⋅], while, if 푡= 휋the series is 1 2휋+ 1 휋[−1 + 1 −1 + ⋅⋅⋅].
Neither of these series are convergent. However, there is a sense of convergence in which the Fourier series of ∑∞ 푛=−∞훿(푡−2푛휋) "converges" to ∑∞ 푛=−∞훿(푡− 2푛휋). To explore this phenomenon, we will explicitly compute the 푛푡ℎpartial sum 훥푛(푡) of the series (8): 훥푛(푡) = 1 2휋+ 1 휋[cos 푡+ cos 2푡+ ⋅⋅⋅+ cos 푛푡] = 1 2휋[1 + 2 cos 푡+ 2 cos2푡+ ⋅⋅⋅+ 2 cos푛푡] Now use the Euler identity 2 cos휃= 푒푖휃+ 푒−푖휃to get 훥푛(푡) = 1 2휋 [ 1 + 푒푖푡+ 푒−푖푡+ 푒푖2푡+ 푒−푖2푡+ ⋅⋅⋅+ 푒푖푛푡+ 푒−푖푛푡] .
Letting 푧= 푒푖푡, this is seen to be a geometric series of ratio 푧that begins with the term 푧−푛and ends with the term 푧푛. Since the sum of a geometric series is known: 푎+ 푎푟+ 푎푟2 + ⋅⋅⋅+ 푎푟푚= 푎(1 −푟푚+1)/(1 −푟) it follows that 훥푛(푡) = 1 2휋 [ 1 + 푒푖푡+ 푒−푖푡+ 푒푖2푡+ 푒−푖2푡+ ⋅⋅⋅+ 푒푖푛푡+ 푒−푖푛푡] = 1 2휋 [ 푧−푛+ 푧−푛+1 + ⋅⋅⋅+ 푧푛] = 1 2휋푧−푛[ 1 + 푧+ ⋅⋅⋅+ 푧2푛] = 1 2휋푧−푛1 −푧2푛+1 1 −푧 = 1 2휋 푧−푛−푧푛+1 1 −푧 = 1 2휋 푒−푖푛푡−푒푖(푛+1)푡 1 −푒푖푡 = 1 2휋 푒푖(푛+1)푡−푒−푖푛푡 푒푖푡−1 푒−푖푡/2 푒−푖푡/2 = 1 2휋 푒푖(푛+ 1 2)푡−푒−푖(푛+ 1 2)푡 푒푖푡/2 −푒−푖푡/2 = 1 2휋 sin ( 푛+ 1 2 ) 푡 sin 1 2푡 .
752 10 Fourier Series For those values of 푡where sin 1 2푡= 0, the value of 훥푛(푡) is the limiting value.
The graphs of 훥푛(푡) for 푛= 5 and 푛= 15 over 1 period −휋≤푡≤휋] are shown in Figure 10.16. As 푛increases the central hump increases in height and becomes narrower, while away from 0 the graph is a rapid oscillation of small amplitude. Also, the area enclosed by 훥푛(푡) in one period −휋≤푡≤휋 is always 1. This is easily seen from the expression of 훥푛(푡) as a sum of cosine terms: ∫휋 −휋 훥푛(푡) 푑푡= ∫휋 −휋 1 2휋[1 + 2 cos푡+ 2 cos2푡+ ⋅⋅⋅+ 2 cos푛푡] 푑푡= 1 since ∫휋 −휋cos 푚푡푑푡= 0 for all nonzero integers 푚. Most of the area is con-centrated in the first hump since the rapid oscillation cancels out the contri-butions above and below the 푡axis away from this hump.
1 2 3 4 5 −1 휋 −휋 훿5(푡) 훿15(푡) Fig. 10.16 The graphs of the partial sums 훿푛(푡) for 푛= 5 and 푛= 15.
To see the sense in which 훥푛(푡) converges to ∑∞ 푛=−∞훿(푡−2푛휋), recall that 훿(푡) is described via integration by the property that 훿(푡) = 0 if 푡∕= 0, and ∫ 푓(푡)훿(푡) 푑푡= 푓(0) for all test functions 푓(푡). Since we are working with periodic functions, consider the integrals over 1 period, in our case [−휋, 휋]. Thus let 푓(푡) be a smooth function and expand it in a cosine series 푓(푡) = ∑푎푚cos 푚푡. Multiply by 훥푛(푡) and integrate, using the orthogonality conditions to get ∫휋 −휋 훥푛(푡)푓(푡) 푑푡= 푎0 + ⋅⋅⋅+ 푎푛.
(9) As 푛→∞this sum converges to 푓(0). Thus 10.3 Convergence of Fourier Series 753 lim 푛→∞ ∫휋 −휋 훥푛(푡)푓(푡) 푑푡= 푓(0) = ∫휋 −휋 훿(푡)푓(푡) 푑푡.
It is in this weak sense that 훥푛(푡) →∑∞ 푛=−∞훿(푡−2푛휋). Namely, the effect under integration is the same.
Exercises 1–9. In each exercise, (a) Sketch the graph of 푓(푡) over at least 3 periods.
(b) Determine the points 푡at which the Fourier series of 푓(푡) converges to 푓(푡). (c) At each point 푡of discontinuity, give the value of 푓(푡) and the value to which the Fourier series converges.
1. 푓(푡) = { 3 if 0 ≤푡< 2 −1 if 2 ≤푡< 4 ; 푓(푡+ 4) = 푓(푡).
2. 푓(푡) = 푡, −1 ≤푡≤1, 푓(푡+ 2) = 푓(푡).
3. 푓(푡) = 푡, 0 ≤푡≤2, 푓(푡+ 2) = 푓(푡).
4. 푓(푡) = ∣푡∣, −1 ≤푡≤1, 푓(푡+ 2) = 푓(푡).
5. 푓(푡) = 푡2, −2 ≤푡≤2, 푓(푡+ 4) = 푓(푡).
6. 푓(푡) = 2푡−1, −1 ≤푡< 1, 푓(푡+ 2) = 푓(푡).
7. 푓(푡) = { 2 if −2 ≤푡< 0 푡 if 0 ≤푡< 2 ; 푓(푡+ 4) = 푓(푡).
8. 푓(푡) = cos(푡/2), 0 ≤푡< 휋, 푓(푡+ 휋) = 푓(푡).
9. 푓(푡) = ∣cos 휋푡∣, 0 ≤푡< 1, 푓(푡+ 1) = 푓(푡).
10. Verify that the following function is not piecewise smooth.
푓(푡) = {√ 푡 if 0 ≤푡< 1 0 if −1 ≤푡< 0.
11. Verify that sin 푡−1 2 sin 2푡+ 1 3 sin 3푡−1 4 sin 4푡+ ⋅⋅⋅= 푡 2, for −휋< 푡< 휋.
Explain how this gives the summation 754 10 Fourier Series 1 −1 3 + 1 5 −1 7 + ⋅⋅⋅= 휋 4 .
12. Use the Fourier series of the function 푓(푡) = ∣푡∣, −휋< 푡< 휋(see Example 4 of Section 10.2) to compute the sum of the series 1 + 1 32 + 1 52 + 1 72 + ⋅⋅⋅.
13. Verify that 1 3 + 4 휋2 ∞ ∑ 푛=1 (−1)푛 푛2 cos 푛휋푡= 푡2, for −1 ≤푡≤1.
14. Using the Fourier series in problem 13, find the sum of the following series ∞ ∑ 푛=1 1 푛2 and ∞ ∑ 푛=1 (−1)푛+1 푛2 .
15. Compute the Fourier series for the function 푓(푡) = 푡4, −휋≤푡≤휋; 푓(푡+ 2휋) = 푓(푡) for all 푡. Using this result, verify the summations ∞ ∑ 푛=1 1 푛4 = 휋4 90 and ∞ ∑ 푛=1 (−1)푛+1 푛4 = 7휋4 720.
10.4 Fourier Sine Series and Fourier Cosine Series In Section 10.2 we observed (see the discussion following Example 5) that the Fourier series of an even function will only have cosine terms, while the Fourier series of an odd function will only have sine terms. We will take advantage of this feature to obtain new types of Fourier series representations that are valid for functions defined on some interval 0 ≤푡≤퐿. In practice, we will frequently want to represent 푓(푡) by a Fourier series that involves only cosine terms or only sine terms. To do this, we will first extend 푓(푡) to the interval −퐿≤푡≤0. We may then extend 푓(푡) to all of the real line by assuming that 푓(푡) is 2퐿periodic. That is, assume 푓(푡+ 2퐿) = 푓(푡). We will extend 푓(푡) in such a way as to obtain either an even function or an odd function.
If 푓(푡) is defined only for 0 ≤푡≤퐿, then the even 2퐿-periodic exten-sion of 푓(푡) is the function 푓푒(푡) defined by 10.4 Fourier Sine Series and Fourier Cosine Series 755 푓푒(푡) = { 푓(푡) if 0 ≤푡≤퐿, 푓(−푡) if −퐿≤푡< 0, ; 푓푒(푡+ 2퐿) = 푓푒(푡).
(1) The odd 2퐿-periodic extension of 푓(푡) is the function 푓표(푡) defined by 푓푒(푡) = { 푓(푡) if 0 ≤푡≤퐿, −푓(−푡) if −퐿≤푡< 0, ; 푓표(푡+ 2퐿) = 푓표(푡).
(2) These two extensions are illustrated for a particular function 푓(푡) in Figure 10.17. Note that both 푓푒(푡) and 푓표(푡) agree with 푓(푡) on the interval 0 < 푡< 퐿.
푦 푡 퐿 The graph of 푓(푡) on the interval 0 ≤푡≤퐿.
푦 푡 퐿 2퐿 3퐿 −퐿 −2퐿 −3퐿 The graph of 푓푒(푡), the even 2퐿-periodic extension of 푓(푡).
푦 푡 퐿 2퐿 3퐿 −퐿 −2퐿 −3퐿 The graph of 푓표(푡), the odd 2퐿-periodic extension of 푓(푡).
Fig. 10.17 Since 푓푒(푡) is an even 2퐿-periodic function, then 푓푒(푡) has a Fourier series expansion 푓푒(푡) ∼푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) where the coefficients are given by Euler’s formulas (Equations (6)-(8) of Section 10.2) 푎0 = 1 퐿 ∫퐿 −퐿 푓푒(푡) 푑푡 756 10 Fourier Series 푎푛= 1 퐿 ∫퐿 −퐿 푓푒(푡) cos 푛휋 퐿푡푑푡, 푛= 1, 2, 3, . . .
푏푛= 1 퐿 ∫퐿 −퐿 푓푒(푡) sin 푛휋 퐿푡푑푡, 푛= 1, 2, 3, . . . .
Since 푓푒(푡) is an even function, then 푓푒(푡) sin 푛휋 퐿푡is odd, so the integral defin-ing 푏푛is 0 (see Proposition 5 of Section 10.1). Thus, 푏푛= 0 and we get the Fourier series expansion 푓푒(푡) ∼푎0 2 + ∞ ∑ 푛=1 푎푛cos 푛휋푡 퐿, where 푎푛= 1 퐿 ∫퐿 −퐿 푓푒(푡) cos 푛휋푡 퐿푑푡, for 푛≥0.
Since the integrand is even and 푓푒(푡) = 푓(푡) for 0 ≤푡≤퐿, it follows that 푎푛= 2 퐿 ∫퐿 0 푓(푡) cos 푛휋푡 퐿푑푡, for 푛≥0.
(3) If we assume that 푓(푡) is piecewise smooth on the interval 0 ≤푡≤퐿, then the even 2퐿-periodic extension 푓푒(푡) is also piecewise smooth, and the con-vergence theorem (Theorem 2 of Section 10.3) shows that the Fourier series of 푓푒(푡) converges to the average of the left-hand and right-hand limits of 푓푒at each 푡. By restricting to the interval 0 ≤푡≤퐿, we obtain the series expansion 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 푎푛cos 푛휋푡 퐿, for 0 ≤푡≤퐿, (4) where the coefficients are given by (3) and this series converges to the average of the left-hand and right-hand limits of 푓at each 푡in the interval [0, 퐿]. The series in (4) is called the Fourier cosine series for 푓on the interval [0, 퐿].
Similarly, by using the Fourier series expansion of the odd 2퐿-periodic extension of 푓(푡), and restricting to the interval 0 ≤푡≤퐿, we obtain the series expansion 푓(푡) ∼ ∞ ∑ 푛=1 푏푛sin 푛휋푡 퐿, for 0 ≤푡≤퐿, (5) where the coefficients are given by 푏푛= 2 퐿 ∫퐿 0 푓(푡) sin 푛휋푡 퐿푑푡, for 푛≥1, (6) 10.4 Fourier Sine Series and Fourier Cosine Series 757 and this series converges to the average of the left-hand and right-hand limits of 푓at each 푡in the interval [0, 퐿]. The series in (5) is called the Fourier sine series for 푓on the interval [0, 퐿].
Example 1. Let 푓(푡) = 휋−푡for 0 ≤푡≤휋. Compute both the Fourier cosine series and the Fourier sine series for the function 푓(푡). Sketch the graph of the function to which the Fourier cosine series converges and the graph of the function to which to Fourier sine series converges.
▶Solution. In this case, the length of the interval is 퐿= 휋and from (4), the Fourier cosine series of 푓(푡) is 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 푎푛cos 푛푡, with 푎0 = 2 휋 ∫휋 0 푓(푡) 푑푡= 2 휋 ∫휋 0 (휋−푡) 푑푡= 휋, and for 푛≥1, 푎푛= 2 휋 ∫휋 0 푓(푡) cos 푛푡푑푡= 2 휋 ∫휋 0 (휋−푡) cos 푛푡푑푡 = 2 푛sin 푛푡 휋 0 −2 휋 ∫휋 0 푡cos 푛푡푑푡 = −2 휋 [ 푡 푛sin 푛푡 휋 0 −1 푛 ∫휋 0 sin 푛푡푑푡 ] = 2 휋푛2 (−cos푛푡) 휋 0 = 2 휋푛2 (−cos 푛휋+ 1) = 2 휋푛2 (1 −(−1)푛) = { 0 if 푛is even, 4 휋푛2 if 푛is odd.
Thus, the Fourier cosine series of 푓(푡) is 푓(푡) = 휋−푡= 휋 2 + 4 휋 ( cos 푡+ 1 32 cos 3푡+ ⋅⋅⋅ 1 (2푘−1)2 cos(2푘−1)푡+ ⋅⋅⋅ ) .
This series converges to 푓(푡) for 0 ≤푡≤휋and to the even 2휋-periodic extension 푓푒(푡) otherwise, since 푓푒(푡) is continuous, as can be seen from the graph of 푓푒(푡) which is given in Figure 10.18.
Similarly, from (5), the Fourier sine series of 푓(푡) is 푓(푡) ∼ ∞ ∑ 푛=1 푏푛sin 푛푡 758 10 Fourier Series 휋 2휋 3휋 −휋 −2휋 −3휋 휋 Fig. 10.18 The even 2휋-periodic extension 푓푒(푡) of the function 푓(푡) = 휋−푡defined on 0 ≤푡≤휋.
with (for 푛≥1) 푏푛= 2 휋 ∫휋 0 푓(푡) sin 푛푡푑푡= 2 휋 ∫휋 0 (휋−푡) sin 푛푡푑푡 = −2 푛cos 푛푡 휋 0 −2 휋 ∫휋 0 푡sin 푛푡푑푡 = −2 푛cos 푛푡 휋 0 −2 휋 [ −푡 푛cos 푛푡 휋 0 + 1 푛 ∫휋 0 cos 푛푡푑푡 ] = 2 푛 Thus, the Fourier sine series of 푓(푡) is 푓(푡) = 휋−푡= 2 ∞ ∑ 푛=1 sin 푛푡 푛 .
This series converges to 푓(푡) for 0 < 푡< 휋and to the odd 2휋-periodic extension 푓표(푡) otherwise, except for the jump discontinuities of 푓표(푡), which occur at the multiples of 푛휋, as can be seen from the graph of 푓표(푡) which is given in Figure 10.19. At 푡= 푛휋, the series converges to 0.
◀ 휋 2휋 3휋 −휋 −2휋 −3휋 휋 −휋 Fig. 10.19 The odd 2휋-periodic extension 푓푒(푡) of the function 푓(푡) = 휋−푡defined on 0 ≤푡≤휋.
10.5 Operations on Fourier Series 759 Exercises 1–11. A function 푓(푡) is defined on an interval 0 < 푡< 퐿. Find the Fourier cosine and sine series of 푓and sketch the graphs of the two extensions of 푓 to which these two series converge.
1. 푓(푡) = 1, 0 < 푡< 퐿 2. 푓(푡) = 푡, 0 < 푡< 1 3. 푓(푡) = 푡, 0 < 푡< 2 4. 푓(푡) = 푡2, 0 < 푡< 1 5. 푓(푡) = { 1 if 0 < 푡< 휋/2 0 if 휋/2 < 푡< 휋 6. 푓(푡) = { 푡 if 0 < 푡≤1, 0 if 1 < 푡< 2 7. 푓(푡) = 푡−푡2, 0 < 푡< 1 8. 푓(푡) = sin 푡, 0 < 푡< 휋 9. 푓(푡) = cos 푡, 0 < 푡< 휋 10. 푓(푡) = 푒푡, 0 < 푡< 1 11. 푓(푡) = 1 −(2/퐿)푡, 0 < 푡< 퐿 10.5 Operations on Fourier Series In applications it is convenient to know how to compute the Fourier series of function obtained from other functions by standard operations such addition, scalar multiplication, differentiation, and integration. We will consider con-ditions under which these operations can be used to facilitate Fourier series calculations. First we consider linearity.
Theorem 1. If 푓and 푔are 2퐿-periodic functions with Fourier series 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) and 760 10 Fourier Series 푔(푡) ∼푐0 2 + ∞ ∑ 푛=1 ( 푐푛cos 푛휋푡 퐿+ 푑푛sin 푛휋푡 퐿 ) , then for any constants 훼and 훽the function defined by ℎ(푡) = 훼푓(푡) + 훽푔(푡) is 2퐿-periodic with Fourier series ℎ(푡) ∼훼푎0 + 훽푐0 2 + ∞ ∑ 푛=1 ( (훼푎푛+ 훽푐푛) cos 푛휋푡 퐿+ (훼푏푛+ 훽푑푛) sin 푛휋푡 퐿 ) . (1) This result follows immediately from the Euler formulas for the Fourier coefficients and from the linearity of the definite integral.
Example 2. Compute the Fourier series of the following periodic functions.
1. ℎ1(푡) = 푡+ ∣푡∣, 휋≤푡< 휋, ℎ1(푡+ 2휋) = ℎ(푡).
2. ℎ2(푡) = 1 + 2푡, −1 ≤푡< 1, ℎ2(푡+ 2) = ℎ(푡).
▶Solution. The following Fourier series were calculated in Examples 4 and 5 of Section 10.2: ∣푡∣= 휋 2 −4 휋 ∞ ∑ 푘=0 cos(2푘+ 1)푡 (2푘+ 1)2 and 푡= 2퐿 휋 ∞ ∑ 푛=1 (−1)푛+1 푛 sin 푛휋 퐿푡.
Since ℎ1 is 2휋-periodic, we take 퐿= 휋in the Fourier series for 푡over the interval 퐿≤푡≤퐿. By the linearity theorem we then obtain ℎ1(푡) = 푡+ ∣푡∣= 휋 2 −4 휋 ∞ ∑ 푘=0 cos(2푘+ 1)푡 (2푘+ 1)2 + 2 ∞ ∑ 푛=1 (−1)푛+1 푛 sin 푛푡.
Since ℎ1(푡) is piecewise smooth, the equality is valid here, with the convention that the function is redefined to be (ℎ1(푡+)+ℎ1(푡−))/2 at each point 푡where the function is discontinuous. The graph of ℎ1(푡) is similar to that of the half sawtooth wave from Figure 10.9, where the only difference is that the period of ℎ1(푡) is 2휋, rather than 4.
The function ℎ2(푡) = 1 + 2푡is a sum of an even function 1 and an odd function 2푡. Since the constant function 1 is it’s own Fourier series (that is, 푎0 = 2, 푎푛= 0 = 푏푛for 푛≥1, then letting 퐿= 1 in the Fourier series for 푡, we get ℎ2(푡) = 1 + 2푡= 1 + 4 휋 ∞ ∑ 푛=1 (−1)푛+1 푛 sin 푛휋푡.
◀ 10.5 Operations on Fourier Series 761 Differentiation of Fourier Series We next consider the term-by-term differentiation of a Fourier series. This will be needed for the solution of some differential equations by substituting the Fourier series of an unknown function into the differential equation. Some care is needed since the term-by-term differentiation of a series of functions is not always valid. The following result gives sufficient conditions for term-by-term differentiation of Fourier series. Note first that if 푓(푡) is a periodic function of period 푝, then the derivative 푓′(푡) (where the derivative exists) is also periodic with period 푝. This follows immediately from the chain rule: Since 푓(푡+ 푝) = 푓(푡) for all 푡, 푓′(푡+ 푝) = 푑 푑푡푓(푡+ 푝) = 푑 푑푡푓(푡) = 푓′(푡).
Theorem 3. Suppose that 푓is a 2퐿-periodic function that is continuous for all 푡, and suppose that the derivative 푓′ is piecewise smooth for all 푡. If the Fourier series of 푓is 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) , (2) then the Fourier series of 푓′ is the series 푓′(푡) ∼ ∞ ∑ 푛=1 ( −푛휋 퐿푎푛sin 푛휋푡 퐿+ 푛휋 퐿푏푛cos 푛휋푡 퐿 ) (3) obtained by term-by-term differentiation of (2). Moreover, the differentiated series (3) converges to 푓′(푡) for all 푡for which 푓′(푡) exists.
Proof. Since 푓′ is assumed to be 2퐿-periodic and piecewise smooth, the con-vergence theorem (Theorem 2 of Section 10.3) shows that the Fourier series of 푓′(푡) converges to the average of the left-hand and right-hand limits of 푓′ at each 푡. That is, 푓′(푡) = 퐴0 2 + ∞ ∑ 푛=1 ( 퐴푛cos 푛휋푡 퐿+ 퐵푛sin 푛휋푡 퐿 ) , (4) where the coefficients 퐴푛and 퐵푛are given by the Euler formulas 퐴푛= 1 퐿 ∫퐿 −퐿 푓′(푡) cos 푛휋푡 퐿푑푡 and 퐵푛= 1 퐿 ∫퐿 −퐿 푓′(푡) sin 푛휋푡 퐿푑푡.
To prove the theorem, it is sufficient to show that the series in Equations (3) and (4) are the same. From the Euler formulas for the Fourier coefficients of 푓′, 762 10 Fourier Series 퐴0 = 1 퐿 ∫퐿 −퐿 푓′(푡) 푑푡= 1 퐿푓(푡)∣퐿 −퐿= 푓(퐿) −푓(−퐿) = 0 since 푓is continuous and 2퐿-periodic. For 푛≥1, the Euler formulas for both 푓′ and 푓, and integration by parts give 퐴푛= 1 퐿 ∫퐿 −퐿 푓′(푡) cos 푛휋푡 퐿푑푡 = 1 퐿푓(푡) cos 푛휋푡 퐿 퐿 −퐿 + 푛휋 퐿⋅1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋푡 퐿푑푡 = 푛휋 퐿푏푛, since 푓(−퐿) = 푓(퐿), and 퐵푛= 1 퐿 ∫퐿 −퐿 푓′(푡) sin 푛휋푡 퐿푑푡 = 1 퐿푓(푡) sin 푛휋푡 퐿 퐿 −퐿 −푛휋 퐿⋅1 퐿 ∫퐿 −퐿 푓(푡) cos 푛휋푡 퐿푑푡 = −푛휋 퐿푎푛.
Therefore, the series in Equations (3) and (4) are the same.
⊓ ⊔ Example 4. The even triangular wave function of period 2휋given by 푓(푡) = { −푡 −휋≤푡< 0, 푡 0 ≤푡< 휋, ; 푓(푡+ 2휋) = 푓(푡), whose graph is shown in Figure 10.7, is continuous for all 푡, and 푓′(푡) = { −1 −휋≤푡< 0, 1 0 < 푡< 휋, ; 푓′(푡+ 2휋) = 푓(푡), is piecewise smooth. In fact 푓′ is an odd square wave of period 2휋as in Figure 10.5. Therefore, 푓satisfies the hypotheses of Theorem 3. Thus, the Fourier series of 푓: 푓(푡) = 휋 2 −4 휋 (cos 푡 12 + cos 3푡 32 + cos 5푡 52 + cos 7푡 72 + ⋅⋅⋅ ) (computed in Example 4 of Section 10.2) can be differentiated term by term.
The result is 푓′(푡) = 4 휋 ( sin 푡+ 1 3 sin 3푡+ 1 5 sin 5푡+ 1 7 sin 7푡+ ⋅⋅⋅ ) , 10.5 Operations on Fourier Series 763 which is the Fourier series of the odd square wave of period 2휋computed in Eq (11) of Section 10.2.
◀ Example 5. The sawtooth wave function of period 2퐿given by 푓(푡) = 푡 for −퐿≤푡< 퐿; 푓(푡+ 2퐿) = 푓(푡).
(see Example 5 of Section 10.2) has Fourier series 푓(푡) ∼2퐿 휋 ( sin 휋 퐿푡−1 2 sin 2휋 퐿푡+ 1 3 sin 3휋 퐿푡−1 4 sin 4휋 퐿푡+ ⋅⋅⋅ ) = 2퐿 휋 ∞ ∑ 푛=1 (−1)푛+1 푛 sin 푛휋 퐿푡.
Since the function 푡is continuous, it might seem that this function satisfies the hypotheses of Theorem 3. However, looking at the graph of the function (see Figure 10.8) shows that the function is discontinuous at the points 푡= ±퐿, 푡= ±3퐿, . . .. Term-by-term differentiation of the Fourier series of 푓gives 2 ( cos 휋 퐿푡−cos 2휋 퐿푡+ cos 3휋 퐿푡−cos 4휋 퐿푡+ ⋅⋅⋅ ) = 2 ∞ ∑ 푛=1 (−1)푛+1 cos 푛휋 퐿푡.
This series does not converge for any point 푡. However, it is possible to make some sense out of this series using the Dirac delta function.
◀ Integration of Fourier Series We now consider the termwise integration of the Fourier series of a piecewise continuous function. Start with a piecewise continuous 2퐿-periodic function 푓and define an antiderivative of 푓by 푔(푡) = ∫푡 −퐿 푓(푥) 푑푥.
(5) Then 푔is a continuous function. It is not automatic that 푔is periodic. How-ever, if 푔(퐿) = ∫퐿 −퐿 푓(푥) 푑푥= 0, (6) it follows that 푔(푡+ 2퐿) = ∫푡+2퐿 −퐿 푓(푥) 푑푥= ∫퐿 −퐿 푓(푥) 푑푥+ ∫푡+2퐿 퐿 푓(푥) 푑푥 764 10 Fourier Series = ∫푡+2퐿 퐿 푓(푥−2퐿) 푑푥 since 푓is 2퐿-periodic = ∫푡 −퐿 푓(푢) 푑푢 using the change of variables 푢= 푥−2퐿 = 푔(푡), so that 푔is periodic of period 2퐿. Therefore we have verified the following result.
Theorem 6. Suppose that 푓is a piecewise continuous 2퐿-periodic function.
Then the antiderivative 푔of 푓defined by (5) is a continuous piecewise smooth 2퐿-periodic function provided that (6) holds.
Now we can state the main result on termwise integration of Fourier series.
Theorem 7. Suppose that 푓is piecewise continuous and 2퐿-periodic with Fourier series 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) .
(7) If 푔(푡) = ∫푡 −퐿푓(푥) 푑푥and 푔(퐿) = ∫퐿 −퐿푓(푥) 푑푥= 0, which is equivalent to 푎0 = 0, then the Fourier series (7) can be integrated term-by-term to give the Fourier series 푔(푡) = ∫푡 −퐿 푓(푥) 푑푥∼퐴0 2 + ∞ ∑ 푛=1 ( 퐿 푛휋푎푛sin 푛휋푡 퐿−퐿 푛휋푏푛cos 푛휋푡 퐿 ) (8) where 퐴0 = −1 퐿 ∫퐿 −퐿 푡푓(푡) 푑푡.
(9) The integrated series (8) converges to 푔(푡) = ∫푡 −퐿푓(푥) 푑푥for all 푡.
Proof. Since 푓is assumed to be 2퐿-periodic and piecewise continuous and 푎0 = 0, Theorem 6 and the convergence theorem shows that the Fourier series of 푔(푡) converges to 푔(푡) at each 푡. That is, 푔(푡) = 퐴0 2 + ∞ ∑ 푛=1 ( 퐴푛cos 푛휋푡 퐿+ 퐵푛sin 푛휋푡 퐿 ) , (10) where the coefficients 퐴푛and 퐵푛are given by the Euler formulas 퐴푛= 1 퐿 ∫퐿 −퐿 푔(푡) cos 푛휋푡 퐿푑푡 and 퐵푛= 1 퐿 ∫퐿 −퐿 푔(푡) sin 푛휋푡 퐿푑푡.
For 푛≥1 apply integration by parts using 푢= 푔(푡), 푑푣= cos 푛휋 퐿푡푑푡so that 푑푢= 푔′(푡) 푑푡= 푓(푡) 푑푡, 푣= 퐿 푛휋sin 푛휋 퐿푡. This gives 10.5 Operations on Fourier Series 765 퐴푛= 1 퐿 ∫퐿 −퐿 푔(푡) cos 푛휋푡 퐿푑푡 = 푔(푡) 1 푛휋sin 푛휋푡 퐿 퐿 −퐿 −1 푛휋 ∫퐿 −퐿 푔′(푡) sin 푛휋푡 퐿푑푡 = −퐿 푛휋 ( 1 퐿 ∫퐿 −퐿 푓(푡) sin 푛휋푡 퐿푑푡 ) .
Hence, 퐴푛= −퐿 푛휋푏푛where 푏푛is the corresponding Fourier coefficient for 푓.
Similarly, 퐵푛= 퐿 푛휋푎푛and using integration by parts with 푢= 푔(푡), 푑푣= 푑푡 so that 푑푢= 푔′(푡) 푑푡= 푓(푡) 푑푡, 푣= 푡, 퐴0 = 1 퐿 ∫퐿 −퐿 푔(푡) 푑푡= 1 퐿푡푔(푡) 퐿 −퐿 −1 퐿 ∫퐿 −퐿 푡푓(푡) 푑푡= −1 퐿 ∫퐿 −퐿 푡푓(푡) 푑푡.
⊓ ⊔ Example 8. Let 푓(푡) be the odd square wave of period 2퐿: 푓(푡) = { −1 −퐿≤푡< 0, 1 0 ≤푡< 퐿, ; 푓(푡+ 2퐿) = 푓(푡), which has Fourier series 푓(푡) ∼4 휋 ( sin 휋 퐿푡+ 1 3 sin 3휋 퐿푡+ 1 5 sin 5휋 퐿푡+ 1 7 sin 7휋 퐿푡+ ⋅⋅⋅ ) that was computed in Eq (11) of Section 10.2. For −퐿≤푡< 0, 푔(푡) = ∫푡 −퐿푓(푥) 푑푥= ∫푡 −퐿(−1) 푑푥= −푡−퐿and for 0 ≤푡< 퐿, 푔(푡) = ∫푡 −퐿푓(푥) 푑푥= ∫0 −퐿(−1) 푑푥+ ∫푡 0 1 푑푥= 푡−퐿. Thus, 푔(푡) is the even triangular wave function of period 2퐿shifted down by 퐿. That is, in the interval −퐿≤푡≤퐿 푔(푡) = ∫푡 −퐿 푓(푥) 푑푥= ∣푡∣−퐿 with 2퐿periodic extension to the rest of the real line. See Figure 10.20.
Theorem 7 then gives, for −퐿≤푡≤퐿, 푔(푡) = ∣푡∣−퐿= 퐴0 2 + 4 휋 ( −퐿 휋cos 휋 퐿푡−퐿 9휋cos 3휋 퐿푡− 퐿 25휋cos 5휋 퐿푡−⋅⋅⋅ ) = 퐴0 2 −4퐿 휋2 ( cos 휋 퐿푡+ 1 9 cos 3휋 퐿푡+ 1 25 cos 5휋 퐿푡+ ⋅⋅⋅ ) 766 10 Fourier Series 푦 푡 1 −1 퐿 2퐿 3퐿 −퐿 −2퐿 −3퐿 (a) 푓(푡) = { −1 −퐿≤푡< 0, 1 0 ≤푡< 퐿.
푦 푡 퐿 −퐿 퐿 2퐿 3퐿 −퐿 −2퐿 −3퐿 (b) 푔(푡) = ∫푡 −퐿푓(푥) 푑푥 Fig. 10.20 = 퐴0 2 −4퐿 휋2 ∞ ∑ 푘=1 1 (2푘−1)2 cos (2푘−1)휋 퐿 푡.
This can also be written as ∣푡∣= ( 퐿+ 퐴0 2 ) −4퐿 휋2 ∞ ∑ 푘=1 1 (2푘−1)2 cos (2푘−1)휋 퐿 푡.
The constant term 퐿+ 퐴0/2 can be determined from Eq. (9): 퐿+ 퐴0 2 = 퐿−1 2퐿 ∫퐿 −퐿 푡푓(푡) 푑푡= 퐿−1 2퐿 ∫퐿 −퐿 ∣푡∣푑푡= 퐿−퐿 2 = 퐿 2 .
The constant term 퐿+ 퐴0/2 can also be determined as one-half of the zero Fourier coefficient of ∣푡∣: 퐿+ 퐴0 2 = 1 2퐿 ∫퐿 −퐿 ∣푡∣푑푡= 퐿 2 .
◀ Exercises 1. Let the 2휋-periodic function 푓1(푡) and 푓2(푡) be defined on −휋≤푡< 휋by 푓1(푡) = 0, −휋≤푡< 0; 푓1(푡) = 1, 0 ≤푡< 휋; 푓2(푡) = 0, −휋≤푡< 0; 푓2(푡) = 푡, 0 ≤푡< 휋.
Then the Fourier series of these functions are 푓1(푡) ∼1 2 + 2 휋 ∑ 푛=odd sin 푛푡 푛 , 10.5 Operations on Fourier Series 767 푓2(푡) ∼휋 4 −2 휋 ∑ 푛=odd cos 푛푡 푛2 + ∞ ∑ 푛=1 (−1)푛+1 sin 푛푡 푛 .
Without further integration, find the Fourier series for the following 2휋-periodic functions: (a) 푓3(푡) = 1, −휋≤푡< 0; 푓3(푡) = 0, 0 ≤푡< 휋; (b) 푓4(푡) = 푡, −휋≤푡< 0; 푓4(푡) = 0, 0 ≤푡< 휋; (c) 푓5(푡) = 1, −휋≤푡< 0; 푓5(푡) = 푡, 0 ≤푡< 휋; (d) 푓6(푡) = 2, −휋≤푡< 0; 푓6(푡) = 0, 0 ≤푡< 휋; (e) 푓7(푡) = 2, −휋≤푡< 0; 푓7(푡) = 3, 0 ≤푡< 휋; (f) 푓8(푡) = 1, −휋≤푡< 0; 푓8(푡) = 1 + 2푡, 0 ≤푡< 휋; (g) 푓9(푡) = 푎+ 푏푡, −휋≤푡< 0; 푓9(푡) = 푐+ 푑푡, 0 ≤푡< 휋.
2. Let 푓1(푡) = 푡for −휋< 푡< 휋and 푓1(푡+ 2휋) = 푓1(푡) so that the Fourier series expansion for 푓1(푡) is 푓1(푡) = 2 ∞ ∑ 푛=1 (−1)푛+1 푛 sin 푛푡.
Using this expansion and Theorem 7 compute the Fourier series of each of the following 2휋-periodic functions.
(a) 푓2(푡) = 푡2 for −휋< 푡< 휋.
(b) 푓3(푡) = 푡3 for −휋< 푡< 휋.
(c) 푓4(푡) = 푡4 for −휋< 푡< 휋.
3. Given that ∣푡∣= 휋 2 −4 휋 ∑ 푛=odd 1 푛2 cos 푛푡, for −휋< 푡< 휋 compute the Fourier series for the function 푓(푡) = 푡2 sgn 푡= { 푡2 if 0 < 푡< 휋 −푡2 if −휋< 푡< 0.
4. Compute the Fourier series for each of the following 2휋-periodic functions.
You should take advantage of Theorem 1 and the Fourier series already computed or given in Exercises 2 and 3.
(a) 푔1(푡) = 2푡−∣푡∣, −휋< 푡< 휋.
(b) 푔2(푡) = 퐴푡2 + 퐵푡+ 퐶, −휋< 푡< 휋, where 퐴, 퐵, and 퐶are constants.
(c) 푔3(푡) = 푡(휋−푡)(휋+ 푡), −휋< 푡< 휋.
5. Let 푓(푡) be the 4-periodic function given by 768 10 Fourier Series 푓(푡) = { −푡 2 if −2 < 푡< 0 푡2 2 −푡 2 if 0 ≤푡< 2.
The Fourier series of 푓(푡) is 푓(푡) ∼−1 3 + 4 휋2 ∞ ∑ 푛=1 ((−1)푛 푛2 cos 푛휋 2 푡+ (−1)푛−1 휋푛3 sin 푛휋 2 푡 ) .
(a) Verify that the hypotheses of Theorem 3 are satisfied for 푓(푡).
(b) Compute the Fourier series of the derivative 푓′(푡).
(c) Verify that the hypotheses of Theorem 3 are not satisfied for 푓′(푡).
10.6 Applications of Fourier Series The applications of Fourier series that will be considered will be applications to differential equations. In this section we will consider finding periodic solu-tions to constant coefficient linear differential equations with periodic forcing function. In the next chapter, Fourier series will be applied to solve certain partial differential equations.
Periodically Forced Differential Equations Example 1. Find all 2휋-periodic solutions of the differential equation 푦′ + 2푦= 푓(푡) (1) where 푓(푡) is a given piecewise smooth 2휋-periodic function.
▶Solution. Since 푓(푡) is piecewise smooth it can be expanded into a Fourier series 푓(푡) = 푎0 2 + ∞ ∑ 푛=1 (푎푛cos 푛푡+ 푏푛sin 푛푡).
(2) If 푦(푡) is a 2휋-periodic solution of (1), then it can also be expanded into a Fourier series 푦(푡) = 퐴0 2 + ∞ ∑ 푛=1 (퐴푛cos 푛푡+ 퐵푛sin 푛푡).
Since 푦(푡) can be differentiated termwise, 푦′(푡) = ∞ ∑ 푛=1 (−푛퐴푛sin 푛푡+ 푛퐵푛cos 푛푡).
10.6 Applications of Fourier Series 769 Now substitute 푦(푡) into the differential equation (1) to get 푦′ + 2푦= ∞ ∑ 푛=1 (−푛퐴푛sin 푛푡+ 푛퐵푛cos 푛푡) + 2 ( 퐴0 2 + ∞ ∑ 푛=1 (퐴푛cos 푛푡+ 퐵푛sin 푛푡) ) = 퐴0 + ∞ ∑ 푛=1 ((2퐴푛+ 푛퐵푛) cos 푛푡+ (2퐵푛−푛퐴푛) sin 푛푡) = 푎0 2 + ∞ ∑ 푛=1 (푎푛cos 푛푡+ 푏푛sin 푛푡).
Comparing coefficients of cos 푛푡and sin 푛푡shows that the coefficients 퐴푛and 퐵푛must satisfy the following equations: 퐴0 = 푎0 2 , and for 푛≥1, 2퐴푛+ 푛퐵푛= 푎푛 −푛퐴푛+ 2퐵푛= 푏푛, (3) which can be solved to give 퐴푛= 2푎푛−푛푏푛 푛2 + 4 and 퐵푛= 푛푎푛+ 2푏푛 푛2 + 4 .
(4) Hence, the only 2휋-periodic solution of (1) has the Fourier series expansion 푦(푡) = 푎0 4 + ∞ ∑ 푛=1 (2푎푛−푛푏푛 푛2 + 4 cos 푛푡+ 푛푎푛+ 2푏푛 푛2 + 4 sin 푛푡 ) .
For a concrete example of this situation, let 푓(푡) be the odd square wave of period 2휋: 푓(푡) = { −1 −휋≤푡< 0, 1 0 ≤푡< 휋, ; 푓(푡+ 2휋) = 푓(푡).
which has Fourier series 푓(푡) = 4 휋 ( sin 푡+ 1 3 sin 3푡+ 1 5 sin 5푡+ 1 7 sin 7푡+ ⋅⋅⋅ ) = 4 휋 ∑ 푛=odd sin 푛푡 푛 .
770 10 Fourier Series Since all of the cosine terms and the even sine terms are 0, (4) gives 퐴푛= 퐵푛= 0 for 푛even, and for 푛odd 퐴푛= −4 휋(푛2 + 4) and 퐵푛= 8 휋푛(푛2 + 4) so that the periodic solution is 푦(푡) = 4 휋 ∑ 푛=odd ( −1 푛2 + 4 cos 푛푡+ 2 푛(푛2 + 4) sin 푛푡 ) .
Rewriting this in phase amplitude form gives 푦(푡) = 4 휋 ∑ 푛=odd 퐶푛cos(푛푡−훿푛) where 퐶푛= √ 퐴2 푛+ 퐵2 푛= 4 휋(푛2 + 4) √ 1 + 4 푛2 .
Thus, computing numerical values gives 퐶1 = 0.5985 퐶3 = 0.1227 퐶5 = 0.0493 퐶7 = 0.0260 퐶9 = 0.0160 The amplitudes are decreasing, but they are decreasing at a slow rate. This is typical of first order equations.
◀ Now consider a second order linear constant coefficient differential equation with 2퐿-periodic forcing function 푎푦′′ + 푏푦′ + 푐푦= 푓(푡), (5) where 푓(푡) is a piecewise continuous 2퐿-periodic with Fourier series 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 ( 푎푛cos 푛휋푡 퐿+ 푏푛sin 푛휋푡 퐿 ) .
(6) To simplify notation, let 휔= 휋/퐿denote the frequency. Then the Fourier series is written as 푓(푡) ∼푎0 2 + ∞ ∑ 푛=1 (푎푛cos 푛휔푡+ 푏푛sin 푛휔푡) .
(7) 10.6 Applications of Fourier Series 771 Assume that there is a 2퐿-periodic solution to (5) that can be expressed in Fourier series form 푦(푡) = 퐴0 2 + ∞ ∑ 푛=1 (퐴푛cos 푛휔푡+ 퐵푛sin 푛휔푡) .
(8) Since 푦′(푡) = ∞ ∑ 푛=1 (−푛휔퐴푛sin 푛휔푡+ 푛휔퐵푛cos 푛휔푡) 푦′′(푡) = ∞ ∑ 푛=1 ( −푛2휔2퐴푛cos 푛휔푡−푛2휔2퐵푛sin 푛휔푡 ) , substituting into the differential equation (5) gives 푎푦′′(푡) + 푏푦′(푡) + 푐푦(푡) = 푐퐴0 2 + ∞ ∑ 푛=1 [(( 푐−푎푛2휔2) 퐴푛+ 푏푛휔퐵푛 ) cos 푛휔푡 + (( 푐−푎푛2휔2) 퐵푛−푏푛휔퐴푛 ) sin 푛휔푡 ] = 푎0 2 + ∞ ∑ 푛=1 (푎푛cos 푛휔푡+ 푏푛sin 푛휔푡) .
(9) Equating coefficients of cos 푛휔푡and sin 푛휔푡leads to equations for 퐴푛and 퐵푛: 푐퐴0 2 = 푎0 2 and for 푛≥1, ( 푐−푎푛2휔2) 퐴푛+ 푏푛휔퐵푛= 푎푛 −푏푛휔퐴푛+ ( 푐−푎푛2휔2) 퐵푛= 푏푛.
(10) This system can be solved for 퐴푛and 퐵푛as long as the determinant of the coefficient matrix is not zero. That is, if 푐−푎푛2휔2 푏푛휔 −푏푛휔 푐−푎푛2휔2 = ( 푐−푎푛2휔2)2 + (푏푛휔)2 ∕= 0.
If 푏∕= 0 this expression is always nonzero, while if 푏= 0 it is nonzero as long as 푛휔∕= √ 푐/푎. These two conditions can be combined compactly into one using the characteristic polynomial 푞(푠) = 푎푠2 + 푏푠+ 푐of the differential equation (5). Note that if 푠= 푖푛휔then 푞(푖푛휔) = 푎(푖푛휔)2 + 푏푖푛휔+ 푐= −푎푛2휔2 + 푖푏푛휔+ 푐.
772 10 Fourier Series Thus, 푞(푖푛휔) ∕= 0 if and only if 푏∕= 0 or 푏= 0 and 푛휔∕= √ 푐/푎. In this case, solving (10) for 퐴푛and 퐵푛(using Cramer’s rule) gives 퐴푛= 푎푛 ( 푐−푎푛2휔2) −푏푛휔푏푛 (푐−푎푛2휔2)2 + (푏푛휔)2 퐵푛= 푏푛 ( 푐−푎푛2휔2) + 푏푛휔푎푛 (푐−푎푛2휔2)2 + (푏푛휔)2 (11) Thus we have arrived at the following result.
Theorem 2. If 푓(푡) is a 2퐿-periodic piecewise continuous function, the dif-ferential equation (5) with characteristic polynomial 푞(푠) has a unique 2퐿-periodic solution whose Fourier series (8) has coefficients computed from those of 푓(푡) by (11), provided that 푞(푖푛휔) ∕= 0 for all 푛≥1.
Example 3. Find all 2-periodic solutions of 푦′′ + 10푦= 푓(푡) (12) where 푓(푡) is the 2-periodic odd square wave function 푓(푡) = { −1 −1 ≤푡< 0, 1 0 ≤푡< 1, ; 푓(푡+ 2) = 푓(푡).
▶Solution. The Fourier series for 푓(푡) is 푓(푡) ∼4 휋 ∑ 푛=odd sin 푛휋푡 푛 .
Since 푛휋∕= 10 for any 푛≥1, there is a unique 2-periodic solution 푦푝(푡) of (12) with Fourier series (whose coefficients are computed from (11)) 푦푝(푡) = 4 휋 ∑ 푛=odd 1 푛(10 −푛2휋2) sin 푛휋푡.
If we calculate the first few terms of this Fourier series we see 푦푝(푡) = 4 휋 ( 1 10 −휋2 sin 휋푡+ 1 3(10 −9휋2) sin 3휋푡+ 1 5(10 −25휋2) sin 5휋푡+ ⋅⋅⋅ ) ∼ = 9.76443 sin휋푡−0.00538 sin3휋푡−0.00108 sin5휋푡−0.00038 sin7휋푡+ ⋅⋅⋅ ∼ = 9.76443 sin휋푡+ (small terms).
Since all the terms in the Fourier series except for the first sine term are extremely small, the effect of the square wave input (forcing function) is an output that is essentially a single sinusoidal term 푦푝(푡) ∼ = 9.76443 sin휋푡.
10.6 Applications of Fourier Series 773 It is typical of second order differential equations to very rapidly reduce the effect of the higher order frequencies of the periodic input (forcing) function.
◀ Example 4. Suppose a mass-spring-dashpot system has mass 푚= 1 kg, spring constant 푘= 25 kg/sec2, damping constant 휇= 0.02 kg/sec, and 2휋-periodic forcing function 푓(푡) defined by 푓(푡) = 휋 2 −∣푡∣, −휋< 푡< 휋.
Thus, the equation of motion is 푦′′ + 0.02푦′ + 25푦= 푓(푡).
(13) Find the unique 2휋-periodic solution 푦(푡) for this problem.
▶Solution. Start by expanding 푓(푡) into a Fourier series (see Example 4 of Section (10.2)): 푓(푡) = 4 휋 (cos 푡 12 + cos 3푡 32 + cos 5푡 52 + cos 7푡 72 + ⋅⋅⋅ ) = 4 휋 ∑ 푛=odd cos 푛푡 푛2 .
(14) The unique 2휋-periodic solution is 푦(푡) = ∑ 푛=odd 퐴푛cos 푛푡+ 퐵푛sin 푛푡 where where coefficients 퐴푛and 퐵푛are computed from (11): 퐴푛= 4(25 −푛2) 푛2휋((25 −푛2)2 + (0.02푛)2) and 퐵푛= 0.08 푛휋((25 −푛2)2 + (0.02푛)2).
Using the phase amplitude formula, each term 푦푛(푡) = 퐴푛cos 푛푡+ 퐵푛sin 푛푡 can be represented in the form 퐶푛sin(푛푡−휃푛) where 퐶푛= √ 퐴2 푛+ 퐵2 푛= 4 푛2휋 √ (25 −푛2)2 + (0.02푛)2 and the solution 푦(푡) can be expressed as 푦(푡) = ∑ 푛=odd 퐶푛sin(푛푡−휃푛).
The first few numerical values of 퐶푛are 774 10 Fourier Series 퐶1 = 0.0530 퐶3 = 0.0088 퐶5 = 0.5100 퐶7 = 0.0011 퐶9 = 0.0003 Thus 푦(푡) ∼ = (0.0530) sin(푡+ 휃1) + (0.0088) sin(3푡+ 휃3) + (0.5100) sin(5푡+ 휃5) + (0.0011) sin(7푡+ 휃7) + (0.0003) sin(9푡+ 휃9) + ⋅⋅⋅.
The relatively large magnitude of 퐶5 is due to the fact that the quantity (25 −푛2)2 + (0.02푛)2 in the denominator is very small for 푛= 5, making (0.5100) sin(5푡+ 휃5) the dominate term in the Fourier series expansion of 푦(푡). Thus, the dominant motion of a spring represented by the differential equation (13) almost a sinusoidal oscillation whose frequency is five times that of the periodic forcing function.
◀ Exercises 1. Let 푓(푡) be the 2-periodic function defined on −1 < 푡< 1 by 푓(푡) = { 0 if −1 < 푡< 0 1 if 0 < 푡< 1 .
Find all 2-periodic solutions to 푦′′ + 4푦= 푓(푡).
2. Find all periodic solutions of 푦′′ + 푦′ + 푦= ∞ ∑ 푛=1 1 푛3 cos 푛푡.
3. Find the general solution of 푦′′ + 푦= ∞ ∑ 푛=1 1 푛2 cos 푛푡 Hint: First solve 푦′′ + 푦= cos 푡by undetermined coefficients. Then let 푓(푡) = ∑∞ 푛=2 푛−2 cos 푛푡and solve 푦′′ + 푦= 푓(푡).
4–7. Find the unique periodic solution of the given differential equation.
10.6 Applications of Fourier Series 775 4. 푦′′ + 3푦= 푓(푡) where 푓(푡) is the 2휋-periodic function defined by 푓(푡) = 5 if 0 < 푡< 휋and 푓(푡) = −5 if 휋< 푡< 0.
5. 푦′′ + 10푦= 푓(푡) where 푓(푡) is the 4-periodic even function defined by 푓(푡) = 5 if 0 < 푡< 1 and 푓(푡) = 0 if 1 < 푡< 2.
6. 푦′′ + 5푦= 푓(푡) where 푓(푡) is the 2-periodic odd function defined by 푓(푡) = 푡if 0 < 푡< 1.
7. 푦′′ + 5푦= 푓(푡) where 푓(푡) is the 2-periodic even function defined by 푓(푡) = 푡if 0 < 푡< 1.
8–10. The values of 푚, 휇, and 푘for a mass-spring-dashpot system are given.
Find the 2퐿-periodic motion expressed in phase amplitude form 푦푝(푡) = 퐴0 2 + ∞ ∑ 푛=1 퐶푛sin(푛휋푡 퐿−휃푛) of the mass under the 2퐿-periodic forcing function 푓(푡). Compute the first three nonzero terms 퐶푛.
8. 푚= 1, 휇= 0.1, 푘= 4; 푓(푡) is the force in Problem 4.
9. 푚= 2, 휇= 0.1, 푘= 18; 푓(푡) is the 2휋-periodic odd function defined by 푓(푡) = 2푡if 0 < 푡< 휋.
10. 푚= 1, 휇= 1, 푘= 10; 푓(푡) is the force in Problem 5. |
11332 | https://brainly.com/question/18887127 | [FREE] Help me or give me answer key plz I’m doing Desmos Quadratic Transformations – Part 1 I’m dum - brainly.com
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Help me or give me answer key plz I’m doing Desmos Quadratic Transformations – Part 1 I’m dum
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In Desmos Quadratic Transformations - Part 1, you can graph quadratic functions and apply different transformations. Common transformations include vertical and horizontal translations, vertical stretching or shrinking, and reflection.
Explanation
Desmos Quadratic Transformations – Part 1
In Desmos, you can graph quadratic functions and apply different transformations to them. The general form of a quadratic function is f(x) = ax^2 + bx + c, where a, b, and c are constants. Here are some common transformations:
Vertical translation: Changing the value of c shifts the graph up or down.
Horizontal translation: Subtracting or adding a constant from x shifts the graph left or right.
Vertical stretching or shrinking: Changing the value of a stretches or shrinks the graph vertically.
Reflection: Changing the sign of a reflects the graph about the x-axis.
Learn more about Desmos Quadratic Transformations here:
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Desmos Quadratic Transformations involve various changes you can apply to quadratic functions like vertical and horizontal translations, stretching or shrinking, and reflections. Each transformation has a specific effect on the graph's shape and position, which you can visually explore in the Desmos platform. Understanding and experimenting with these transformations will enhance your graphing skills for quadratic functions.
Explanation
In Desmos Quadratic Transformations – Part 1, you'll be learning how to graph quadratic functions and apply various transformations to them. A quadratic function usually has the form:
f(x)=a x 2+b x+c where a, b, and c are constants. The types of transformations include:
Vertical translation: This is done by changing the value of c. For example, if you have the function
f(x)=x 2
and change it to
f(x)=x 2+3
the graph shifts up by 3 units.
Horizontal translation: This involves adding or subtracting a constant from x. For instance, changing the function from
f(x)=x 2
to
f(x)=(x−2)2
shifts the graph to the right by 2 units, while
f(x)=(x+2)2
moves it to the left by 2 units.
Vertical stretching or shrinking: Altering the coefficient a. For example,
f(x)=2 x 2
will stretch the graph vertically, making it narrower, while
f(x)=0.5 x 2
will compress it, making it wider.
Reflection: Changing the sign of a reflects the graph across the x-axis. For example,
f(x)=−x 2
flips the graph of
f(x)=x 2
downwards.
Understanding these transformations can greatly help you in graphing and analyzing quadratic functions in Desmos. Make sure to experiment with the values in the platform to see how each transformation affects the graph visually.
Happy graphing!
Examples & Evidence
For example, if you start with the function f(x) = x² and modify the equation to f(x) = (x - 3)², this results in a shift of the graph to the right by 3 units. Similarly, changing f(x) = x² to f(x) = 2x² scales the graph vertically, making it narrower.
These mathematical transformations can be found in any algebra or precalculus textbook regarding quadratic equations, and platforms like Desmos provide interactive ways to visualize these concepts.
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While the slider moves to the right the point change also. You can see that the points will decrease and increase again.
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11333 | https://physics.stackexchange.com/questions/652301/what-has-eulers-number-e-to-do-with-exponential-decay | Stack Exchange Network
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What has Euler's number $e$ to do with exponential decay?
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$\begingroup$
I know how to derive the formula for "quantity at time $t$" for some decaying materials. You can see the derivation here. But, what I don't get is that what the number $e$ is doing here? We get the value of $e$ from the equation of compound interest. Compound interest and decay (like, radioactive decay) are two different things. Is there any intuitive way to see what the Euler's number doing here?
radiation
radioactivity
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edited Jul 19, 2021 at 16:11
Qmechanic♦
222k5252 gold badges636636 silver badges2.6k2.6k bronze badges
asked Jul 19, 2021 at 16:07
user307064user307064
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4
2
$\begingroup$ It's not clear what you're asking. You seem to understand the derivation and that this is the solution to the equation. What more of an answer do you want than that? $\endgroup$
Brick
– Brick
2021-07-19 16:09:51 +00:00
Commented Jul 19, 2021 at 16:09
1
$\begingroup$ Compound interest is exponential growth. Radioactivity is exponential decay. Same math, just backwards. $\endgroup$
Jon Custer
– Jon Custer
2021-07-19 16:10:08 +00:00
Commented Jul 19, 2021 at 16:10
3
$\begingroup$ This question is about math or possibly the history of math, but not physics $\endgroup$
Paul T.
– Paul T.
2021-07-19 16:15:04 +00:00
Commented Jul 19, 2021 at 16:15
$\begingroup$ You question is either unclear or it should be asked in Math SE. If you are asking why we have $e^{\lambda t}$ and not some other number say $a^{\lambda t}$ when it belongs to Math SE. $\endgroup$
TheImperfectCrazy
– TheImperfectCrazy
2021-07-19 16:25:46 +00:00
Commented Jul 19, 2021 at 16:25
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3 Answers 3
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$\begingroup$
Compound interest and radioactive decay both vary exponentially with time. That simply means that in any set period of time, the value changes by the same fractional amount.
Any exponential function can be written using any base. If the number of remaining atoms in a sample is given by $A e^{-Bt}$, then it is also given by $A 2^{-Ct}$, for the appropriate value of $C$.
Regardless of the base you choose, the number $e$ pops out when you calculate the rate of change of the exponential function (which is another exponential function). So, assuming you are interested in, say, both the number of atoms and how fast that number is changing, you will be stuck with an $e$ somewhere or other anyway. Choosing it as the base eliminates a constant that would otherwise appear in the expressions.
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answered Jul 19, 2021 at 16:39
Ben51Ben51
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$\endgroup$
1
2
$\begingroup$ In fact, the $2^{-t/t_{1/2}}$ is quite a natural way to express the decay in terms of half-life. $\endgroup$
Ruslan
– Ruslan
2021-07-19 17:02:23 +00:00
Commented Jul 19, 2021 at 17:02
Add a comment |
4
$\begingroup$
By definition, the natural log base $\mathrm{e}$ has the special property that
$$ \tfrac{\rm d}{{\rm d}t} \mathrm{e}^t = \mathrm{e}^t $$
This leads us to understand that all solutions to
$$ \tfrac{\rm d}{{\rm d}t} f(t) = f(t) $$ have basis functions $f(t) \propto \mathrm{e}^t$.
A subset of these problems are that of
$$ \tfrac{\rm d}{{\rm d}t} x(t) = -a\, x(t) $$ which have solutions of the form $x(t) = X \mathrm{e}^{-a t}$
This is the basic exponential decay formula, and the interpretation of the differential equation is that the amount decaying is proportional to the amount that exists at any time.
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edited Jul 19, 2021 at 19:28
answered Jul 19, 2021 at 16:56
jalexjalex
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$\begingroup$ As an aside, imo it is important to mention that this is the reason why we cared to talk about $e$ in the first place. When we calculate the derivative of $a^x$, it comes out to be $ka^x$. A natural question to ask is, for what number $a$ is the constant $k=1$. That is the Euler's number $e$, and the constant thus becomes $\ln(e)$. $\endgroup$
Physiker
– Physiker
2021-07-19 18:30:47 +00:00
Commented Jul 19, 2021 at 18:30
1
$\begingroup$ @IndischerPhysiker - of course and that is what I was trying to convey in my first sentence. The value of $\mathrm{e}$ is special as it allows the derivative to be equal to the value. $\endgroup$
jalex
– jalex
2021-07-19 19:28:07 +00:00
Commented Jul 19, 2021 at 19:28
Add a comment |
-1
$\begingroup$
Compound interest is exponential decay when you examine it closely.
Look at e in the formula for compound interest: (1 + 1/n)^n
Look at the fraction 1/n. The larger n gets, the smaller the fraction gets. In fact, it gets exponentially smaller. Exponential decay.
In the infinite sum for the compound interest equation above, the larger n gets, the closer it gets to e. If you let n run to infinity, the answer would converge to e. An easy way to see this is to set principal to $1.00, interest rate to 100%, and compounding periods to fractions of one year i.e. for compounded every six months would be (1+ 1/2)^2. Then try higher and higher numbers for n. The return on principal plus principal approaches e. Exponential decay of return.
In fact, when you graph the compound interest formula, it looks like a reflection of e^x ( See Wolfram Alpha on the constant e).
Eulers number has to do with exponentials. All constants to a time exponential, have a derivative that has a proportionality constant. When the proportionality constant is the number 1, the constant is e.
However, it should be understood that the compound interest formula has a limit of e, whereas, the function e^-x has a limit of zero. And it should be understood that many infinite series can converge to a real number. To understand why e (Eulers number) is special, see YouTube by 3Blue1Brown called Whats so special about Eulers number e?
If you invest your money, the rate at which it grows is proportional to the amount of money there at any time. In all of these cases where some variables rate of change is proportional to itself, the function describing that variable over time is going to look like some kind of exponential. And even though there are lots of ways to write any exponential function, it is very natural to choose to express these functions as e to the power of some constant times t since that constant carries a very natural meaning. Its the same as the proportionality constant between the size of the changing variable and the rate of change.Grant Sanderson
But if you are asking Why? e shows up in biology, math(s), compound interest, radioactive decay, etc., that is like asking why pi shows up in population growth and many other functions when it comes from a circle formula. Most of Science cant answer Why? They can measure observations, predict from observations with mathematical principles, but cannot yet answer why? IMHO, someday they will.
The more interesting question is if radioactive decay has a predictable half-life, how can it be spontaneous i.e. meaning random decay without a pattern in the individual atom. Quantum Physics cannot yet answer this. They can measure decay in half-lives, but they also can mathematically explain spontaneous emission. How does something random form a pattern?
BTW, physics cannot really be separated from mathematics, so your question is a physics question.
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edited Dec 3, 2022 at 20:39
answered Dec 2, 2022 at 15:34
VoyajerVoyajer
111 bronze badge
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$\begingroup$ (1) $1/n$ does not get exponentially smaller with increasing $n$. (2) Its perfectly reasonable to ask why $\pi$ shows up all over the place, and the answers usually relate to $\pi$ being half of the period of the complex exponential function $e^{ix}$. It's also perfectly reasonable to ask the same question of $e$. Such questions are better phrased as e.g. "how does $e$ arise in this expression?" and are distinct from the "why" questions which science is unable to answer. (3) Random events can be often be described by probability distributions, and can still be studied mathematically. $\endgroup$
Albatross
– Albatross
2022-12-03 20:04:35 +00:00
Commented Dec 3, 2022 at 20:04
$\begingroup$ (4) Physics and mathematics are completely different enterprises which share a common language, so physics and mathematics can absolutely be separated - at least in some cases. Not every mathematical question relates to physics. $\endgroup$
Albatross
– Albatross
2022-12-03 20:04:39 +00:00
Commented Dec 3, 2022 at 20:04
$\begingroup$ You can do math for maths sake, but you cant do physics without math and a question about radioactive decay is physics. Eulers number e is defined by the compound interest formula. It is defined by the infinite fraction that can be created by the formula. It is also defined by the infinite series found by Newton. It is also defined by the exponential proportionality constant. Euler found that e to the x contains the infinite series for sines and cosines multiplied by the imaginary number i. When you have a number that is defined by something, you cant answer why. $\endgroup$
Voyajer
– Voyajer
2022-12-04 12:47:05 +00:00
Commented Dec 4, 2022 at 12:47
$\begingroup$ (1) All fractions get smaller by increasing the denominator. Basic arithmetic. Think again. (2) Especially if they have the same exponent as the denominator, they get exponentially smaller. $\endgroup$
Voyajer
– Voyajer
2022-12-04 12:56:59 +00:00
Commented Dec 4, 2022 at 12:56
$\begingroup$ Exponentially smaller generally means that something goes like $a^{-n}$ for some positive number $a$. $1/n$ does not qualify; you might call it inverse-linear or something to that effect, but exponential has a specific meaning. In any case, any answer to why $e$ is present in the formula for exponential decay is purely one based on convention, since $N(t)=N_0 2^{-t/T}$ works just as well (and actually better when we're talking about decay in terms of half-lives). $\endgroup$
Albatross
– Albatross
2022-12-04 14:54:34 +00:00
Commented Dec 4, 2022 at 14:54
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11334 | https://www.youtube.com/watch?v=tZKzaF28sOk | Polynomial end behavior | Polynomial and rational functions | Algebra II | Khan Academy
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Transcript:
What I want to do in this
video is talk a little bit about polynomial end behavior. And this is really
just talking about what happens to a polynomial if
as x becomes really large or really, really,
really negative. For example, we're familiar
with quadratic polynomials where y is equal to ax
squared plus bx plus c. We know that if a
is greater than 0, this is going to be an upward
opening parabola of some kind. So it's going to look
something like that, the graph of this equation,
or of this function, you could say. And if a is less
than 0, it's going to be a downward
opening parabola. We've spent less time with
third degree polynomials, but we've also seen
those a little bit. So for example, if you have
the third degree polynomial, y is equal to ax to the third
plus bx squared plus cx plus d, if a is greater than 0-- I don't
want to use that brown color. If a is greater than 0,
when x is really, really, really negative, this whole
thing is going to be really, really, really negative. And then it's going to increase
as x becomes less negative. It's going do
something-- it might do a little bit of
funky stuff in between. But then as x becomes more
and more and more positive, it will become more and more
and more positive as well. So it might look something like
this when a is greater than 0. But what about when
a is less than 0? Well then, just like
here, we would flip it. We would flip it so that
if a is less than 0, when x is really
negative, you're going to multiply that
times a negative a and you're going to
get a positive value. So it's going to look
something like this. And then it's going
to go like this. It might do a little bit of this
type of business in between. But then its end behavior,
it starts decreasing again. It starts decreasing. So when we talk
about end behavior, we're talking about the idea
of what is this function? What does this polynomial do
as x becomes really, really, really, really positive
and as x becomes really, really, really, really negative? And kind of fully recognizing
that some weird things might be happening in the middle. But we just want
to think about what happens at extreme values of x. Now obviously for
the second degree polynomial nothing really
weird happens in the middle. But for a third
degree polynomial, we sort of see that
some interesting things can start happening
in the middle. But the end behavior for
third degree polynomial is that if a is
greater than 0-- we're starting really small,
really low values-- and as a becomes positive,
we get to really high values. If a is less than 0
we have the opposite. And these are kind of the two
prototypes for polynomials. Because from there we can
start thinking about any degree polynomial. So let's just think about the
situation of a fourth degree polynomial. So let's say y is equal
to ax to the fourth power plus bx to the third plus cx
squared plus dx plus-- I don't want to write e because e has
other meanings in mathematics. I'll say plus-- I'm really
running out of letters here. I'll just use f, although
this isn't the function f. This is just a constant
f right over here. So let's just think about
what this might look like. Let's think about
its end behavior, and we could think about it
relative to a second degree polynomial. So its end behavior, if x is
really, really, really, really negative, x to the fourth is
still going to be positive. And if a is greater than 0
when x is really, really, really negative, we're
going to have really, really positive values, just
like a second degree. And when x is really
positive, same thing. x to the fourth is
going to be positive, times a is still
going to be positive. So its end behavior
is going to look very similar to a second
degree polynomial. Now, it might do--
in fact it probably will do some funky
stuff in between. It might do something that looks
kind of like that in between. But we care about
the end behavior. I guess you could call
the stuff that I've dotted lined in the middle, this is
called the non-end behavior, the middle behavior. This will obviously be
different than a second degree polynomial. But what happens at the
ends will be the same. And the reason why, when
you square something, or you raise something
to the fourth power, you raise anything to any even
power for a very large-- as long as a is greater than 0,
for very large positive values, you're going to get
positive values. And for very large
negative values, you're going to get very
large positive values. You take a negative number,
raise it to the fourth power, or the second power, you're
going to get a positive value. Likewise, if a is
less than 0, you're going to have very similar
end behavior to this case. For a polynomial where
the highest degree term is even-- so this is
a is less than 0-- your end behavior when a is really,
really, really, really negative, this thing
is going to be really, really, really positive. We're going to be multiplying
it times a negative, so it's going to
be really, really, really, really negative. So it'll look like this. And likewise, when x is really,
really, really positive, you get the same thing. Because you're going to be
multiplying a positive times a, which is negative,
and in between it might be doing
something like that. But its end
behavior, you see, is very similar to a second
degree polynomial. So if you ignore this, its
end behavior is very similar. Now the same is true
for a fifth degree if you were to compare
it to a third degree. And the overall idea here is
what happens to this value when we get really large x's
or really small x's? Are we taking it
to an even power? In which case for either really
negative values or really positive values we're going
to get positive values. And then it depends what
our coefficient a is. Or are we taking
it to an odd power? So the general
idea-- and actually let me just do a fifth degree,
just to make the clear. So if I had something
of the form y is equal to ax to the fifth
plus bx to the fourth plus-- and it just went all the way--
I won't even have to write it. This thing, if a
is greater than 0, would look something like this. Its end behavior is very similar
to a third degree polynomial where a is greater than 0. At the end it would do this. Now, it might do kind of
some craziness like this. I have to get this right. So 1, 2, 3-- it might do some
craziness like this in between. But then for really large x's
it will look the same as ax to the third when a
is greater than 0. So once again, very,
very similar end behavior when a is greater than
0, and very similar end behavior when
a is less than 0. It would look like this. At the ends at a
negative value it will be positive
because this part is going to be really negative. But then it's going to be
multiplied by a negative to get a positive. And for really positive values
of x, it will be negative. Because once again, this a
term is going to be negative. And then what it does
in between-- at least for the sake of
this video-- we're not really thinking about. So the big takeaway
here-- and this is kind of a little
bit of a drum roll here, we're talking
about end behavior-- if you're looking at an
even degree polynomial it's going to have end
behavior like a second degree polynomial. If you ignore what happens
in the middle, what happens at really negative
values of x and really positive values of x is going to be
very similar to a second degree polynomial. And if your degree
is odd, you're going to have very similar
end behavior to a third degree polynomial. You might do all sorts of
craziness in the middle, but given for a given a,
whether it's greater than 0 or less than 0, you will
have end behavior like this, or end behavior like that. |
11335 | https://www.youtube.com/watch?v=q12ABN6BQLo | Quadratic Inequality | x²+3x-4 greater than 0
Tambuwal Maths Class
313000 subscribers
30 likes
Description
1208 views
Posted: 1 Mar 2024
To solve x² + 3x - 4 greater than 0, you can first find the roots by setting it equal to zero: x² + 3x - 4 = 0.
we can factorize x² + 3x - 4 to find its roots.
Thus (x + 4)(x - 1).
Setting each factor equal to zero gives us the roots:
x = -4 or x = 1
Now, we have the roots x = -4 and x = 1. We can use these roots to determine the intervals where x² + 3x - 4 is greater than 0
5 comments
Transcript:
Introduction hello good day viewers still on quadratic inequalities today I'm going to show you how to solve quadratic inequalities by graphing if at all you don't want to use number line to test some values so if you new here consider subscribing press the Bell icon so that you will be notified whenever I upload a new content and don't forget to share to your learning colleagues all right let's Quadratic Inequality get started we have a quadratic inequality here you can see that they are exactly the same just that this is greater than five and this is less than five so let us pay attention to the first one here um let us try to factorize this because it is factorable think of two numbers you can multiply together to get -4 but once you add the two numbers together you shall obtain three and the numbers are -1 and POS 4 because 4 -1 will give us -4 and 4 + -1 is the same thing as 4 - 1 which is 3 so we can write this as x + 4 then um X - 1 greater than 0 you know the roots will be -4 and positive one the moment you take four and negative one to the other side of the inequality they will change sign this will become negative and this will be positive so if I have y and x axis like this we shall locate -4 here this is4 to the left and positive one will be somewhere here right and because the quadratic expression has its leading coefficient to be positive you should expect what an open up Parabola so it will be something like this something like this right all right I remember our inequality is GRE greater than Ty and the whole left hand side remember it is representing y right because you know we used to write a quadratic equation as y = a x^ 2 + b x + C so the whole of this expression is representing y so here we are saying that the of y greater than Z so why do we have y greater than Z from the origin here and everything to the top and at what value of X is why said to be positive is what at -4 and Why everything to the left hand side you can see them all vales to the left hand side because the moment you take a value here it is going to hit the parabola somewhere here where Y is negative right so we only expect from -4 way down to negative infinity and from one way down to positive Infinity that is the only place you could get a value of x substituted into the expression and the value of y will be greater than zero so our solution here Solution will be what um x value that will satisfy will be a value from negative Infinity we down to4 excluding because the inequality is just greater than but supp it is greater or equal to we have to include by using square brackets something like this then Union We join the other solution from one way down to positive infinity and this is said to be the solution to this problem but what about in a case where we have less than zero you can see that all this portion is where you have y to be negative so we expect everything from -4 down to one that's where you're going to get the solution so for this one since Outro the expressions are exactly the same just that they have difference of inequality this will have a solution from -4 down to positive one and that's just the difference between them thank you for watching do share to your learning colleagues and don't forget to subscribe to my YouTube channel for more exciting videos [Music] bye-bye |
11336 | https://www.nice.org.uk/guidance/ng100/resources/rheumatoid-arthritis-in-adults-management-pdf-66141531233989 | Rheumatoid arthritis in
adults: management
NICE guideline
Published: 11 July 2018
Last updated: 12 October 2020
www.nice.org.uk/guidance/ng100
© NICE 2025. All rights reserved. Subject to Notice of rights ( Your responsibility
The recommendations in this guideline represent the view of NICE, arrived at after careful
consideration of the evidence available. When exercising their judgement, professionals
and practitioners are expected to take this guideline fully into account, alongside the
individual needs, preferences and values of their patients or the people using their service.
It is not mandatory to apply the recommendations, and the guideline does not override the
responsibility to make decisions appropriate to the circumstances of the individual, in
consultation with them and their families and carers or guardian.
All problems (adverse events) related to a medicine or medical device used for treatment
or in a procedure should be reported to the Medicines and Healthcare products Regulatory
Agency using the Yellow Card Scheme .
Local commissioners and providers of healthcare have a responsibility to enable the
guideline to be applied when individual professionals and people using services wish to
use it. They should do so in the context of local and national priorities for funding and
developing services, and in light of their duties to have due regard to the need to eliminate
unlawful discrimination, to advance equality of opportunity and to reduce health
inequalities. Nothing in this guideline should be interpreted in a way that would be
inconsistent with complying with those duties.
Commissioners and providers have a responsibility to promote an environmentally
sustainable health and care system and should assess and reduce the environmental
impact of implementing NICE recommendations wherever possible.
Rheumatoid arthritis in adults: management (NG100)
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Contents
Overview .................................................................................................................................. 5
Who is it for? ....................................................................................................................................... 5
Recommendations ................................................................................................................... 6
1.1 Referral, diagnosis and investigations ......................................................................................... 6
1.2 Treat-to-target strategy .............................................................................................................. 8
1.3 Communication and education ................................................................................................... 8
1.4 Initial pharmacological management .......................................................................................... 9
1.5 Further pharmacological management ...................................................................................... 10
1.6 Symptom control .......................................................................................................................... 14
1.7 The multidisciplinary team ........................................................................................................... 15
1.8 Non-pharmacological management ........................................................................................... 15
1.9 Monitoring ..................................................................................................................................... 17
1.10 Timing and referral for surgery .................................................................................................. 19
Terms used in this guideline .............................................................................................................. 20
Recommendations for research ............................................................................................. 22
Key recommendations for research ................................................................................................. 22
Other recommendations for research .............................................................................................. 25
Rationale and impact ............................................................................................................... 26
Investigations following diagnosis .................................................................................................... 26
Investigations (ultrasound in diagnosis) .......................................................................................... 27
Treat-to-target strategy .................................................................................................................... 27
DMARDs .............................................................................................................................................. 29
Short-term bridging treatment with glucocorticoids ...................................................................... 32
Symptom control ................................................................................................................................ 33
Monitoring ........................................................................................................................................... 34
Context ..................................................................................................................................... 36
Finding more information and committee details ................................................................. 37
Rheumatoid arthritis in adults: management (NG100)
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Update information ................................................................................................................. 38
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This guideline replaces CG79.
This guideline is the basis of QS33.
This guideline should be read in conjunction with NG193.
Overview
This guideline covers diagnosing and managing rheumatoid arthritis. It aims to improve
quality of life by ensuring that people with rheumatoid arthritis have the right treatment to
slow the progression of their condition and control their symptoms. People should also
have rapid access to specialist care if their condition suddenly worsens.
Who is it for?
• Healthcare professionals
• Commissioners and providers
• People with rheumatoid arthritis and their families and carers
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Page 5 of 39 Recommendations
People have the right to be involved in discussions and make informed decisions
about their care, as described in making decisions about your care .
Making decisions using NICE guidelines explains how we use words to show the
strength (or certainty) of our recommendations, and has information about
prescribing medicines (including off-label use), professional guidelines, standards
and laws (including on consent and mental capacity), and safeguarding.
1.1 Referral, diagnosis and investigations
Referral from primary care
1.1.1
Refer for specialist opinion any adult with suspected persistent synovitis of
undetermined cause. Refer urgently (even with a normal acute-phase response,
negative anti-cyclic citrullinated peptide [CCP] antibodies or rheumatoid factor) if
any of the following apply:
• the small joints of the hands or feet are affected
• more than one joint is affected
• there has been a delay of 3 months or longer between onset of symptoms
and seeking medical advice. [2009, amended 2018]
Investigations
If the following investigations are ordered in primary care, they should not delay referral for
specialist opinion (see recommendation 1.1.1).
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Investigations for diagnosis
1.1.2
Offer to carry out a blood test for rheumatoid factor in adults with suspected
rheumatoid arthritis (RA) who are found to have synovitis on clinical examination.
1.1.3
Consider measuring anti-CCP antibodies in adults with suspected RA if they are
negative for rheumatoid factor. [2009, amended 2018]
1.1.4
X-ray the hands and feet in adults with suspected RA and persistent synovitis.
[2009, amended 2018]
Investigations following diagnosis
1.1.5
As soon as possible after establishing a diagnosis of RA:
• measure anti-CCP antibodies, unless already measured to inform diagnosis
• X-ray the hands and feet to establish whether erosions are present, unless X-
rays were performed to inform diagnosis
• measure functional ability using, for example, the Health Assessment
Questionnaire (HAQ), to provide a baseline for assessing the functional
response to treatment.
1.1.6
If anti-CCP antibodies are present or there are erosions on X-ray:
• advise the person that they have an increased risk of radiological progression
but not necessarily an increased risk of poor function, and
• emphasise the importance of monitoring their condition, and seeking rapid
access to specialist care if disease worsens or they have a flare.
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For a short explanation of why the committee made the 2018 recommendations and
how they might affect practice, see the rationale and impact section on investigations
following diagnosis .
Full details of the evidence and the committee's discussion are in evidence review B:
Risk factors .
1.2 Treat-to-target strategy
1.2.1
Treat active RA in adults with the aim of achieving a target of remission or low
disease activity if remission cannot be achieved ( treat-to-target ). Achieving the
target may involve trying multiple conventional disease-modifying anti-rheumatic
drugs (cDMARDs), and biological or targeted synthetic DMARDs with different
mechanisms of action, one after the other. [2018, amended 2024]
1.2.2
Consider making the target remission rather than low disease activity for people
with an increased risk of radiological progression (presence of anti-CCP
antibodies or erosions on X-ray at baseline assessment).
1.2.3
In adults with active RA, measure C-reactive protein (CRP) and disease activity
(using a composite score such as DAS28) monthly in specialist care until the
target of remission or low disease activity is achieved.
For a short explanation of why the committee made the 2018 recommendations and
how they might affect practice, see the rationale and impact section on treat-to-
target strategy .
Full details of the evidence and the committee's discussion are in evidence review C:
Treat-to-target .
1.3 Communication and education
1.3.1
Explain the risks and benefits of treatment options to adults with RA in ways that
can be easily understood. Throughout the course of their disease, offer them the
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opportunity to talk about and agree all aspects of their care, and respect the
decisions they make.
1.3.2
Offer verbal and written information to adults with RA to:
• improve their understanding of the condition and its management, and
• counter any misconceptions they may have. [2009 ]
1.3.3
Adults with RA who wish to know more about their disease and its management
should be offered the opportunity to take part in existing educational activities,
including self-management programmes.
1.4 Initial pharmacological management
Conventional disease-modifying anti-rheumatic drugs
1.4.1
For adults with newly diagnosed active RA:
• Offer first-line treatment with cDMARD monotherapy using oral methotrexate,
leflunomide or sulfasalazine as soon as possible and ideally within 3 months
of onset of persistent symptoms.
• Consider hydroxychloroquine for first-line treatment as an alternative to oral
methotrexate, leflunomide or sulfasalazine for mild or palindromic disease.
• Escalate dose as tolerated.
1.4.2
Consider short-term bridging treatment with glucocorticoids (oral, intramuscular
or intra-articular) when starting a new cDMARD.
For a short explanation of why the committee made the 2018 recommendations and
how they might affect practice, see the rationale and impact section on short-term
bridging treatment with glucocorticoids .
Full details of the evidence and the committee's discussion are in evidence review H:
Glucocorticoids .
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Page 9 of 39 1.4.3
Offer additional cDMARDs (oral methotrexate, leflunomide, sulfasalazine or
hydroxychloroquine) in combination in a step-up strategy when the treatment
target (remission or low disease activity) has not been achieved despite dose
escalation.
For a short explanation of why the committee made the 2018 recommendations and
how they might affect practice, see the rationale and impact section on DMARDs .
Full details of the evidence and the committee's discussion are in evidence review F:
DMARDs .
1.5 Further pharmacological management
For guidance on using DMARDs to achieve treatment targets, see section 1.2.1 . Also see
the MHRA's safety advice on Janus kinase (JAK) inhibitors (April 2023) .
See terms used in this guideline for a description and examples of tumour necrosis factor
(TNF) inhibitors and JAK inhibitors .
Biological and targeted synthetic DMARDs
1.5.1
If people with RA and their clinicians consider there to be a range of suitable
medicines, after discussing the advantages and disadvantages of all the options,
the least expensive should be used. Administration costs, dosages, price per
dose and commercial arrangements should all be taken into account.
Moderate RA
1.5.2
For medicines recommended as options in NICE technology appraisal guidance
for treating moderate RA (disease activity score [DAS28] of 3.2 to 5.1) that has
inadequately responded to intensive therapy with 2 or more conventional
DMARDs (cDMARDs) used in combination, see the guidance on:
• upadacitinib (TA744, November 2021)
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• adalimumab (TA715, July 2021)
• etanercept (TA715, July 2021)
• infliximab (TA715, July 2021)
• filgotinib (TA676, July 2021) .
Give the biological or targeted synthetic DMARD in combination with
methotrexate unless it is contraindicated, or the person cannot tolerate it.
Infliximab is not recommended for monotherapy.
Severe RA
1.5.3
For medicines recommended as options in NICE technology appraisal guidance
for treating severe RA (DAS28 of more than 5.1) that has inadequately responded
to intensive therapy with conventional DMARDs (cDMARDs) used in combination,
see the guidance on:
• filgotinib (TA676, February 2021)
• upadacitinib (TA665, December 2020)
• sarilumab (TA485, November 2017)
• tofacitinib (TA480, October 2017)
• baricitinib (TA466, August 2017)
• abatacept (TA375, January 2016)
• adalimumab (TA375, January 2016)
• certolizumab pegol (TA375, January 2016)
• etanercept (TA375, January 2016)
• golimumab (TA375, January 2016)
• infliximab (TA375, January 2016)
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• tocilizumab (TA375, January 2016) .
Give the biological or targeted synthetic DMARD in combination with
methotrexate unless it is contraindicated, or the person cannot tolerate it.
Abatacept, golimumab and infliximab are not recommended for monotherapy.
1.5.4
Rituximab in combination with methotrexate is recommended as an option in
NICE technology appraisal guidance for treating severe RA (DAS28 of more than
5.1) that has inadequately responded to at least 1 TNF inhibitor . For full details,
see the guidance on rituximab (TA195, August 2010) .
1.5.5
For medicines recommended as options in NICE technology appraisal guidance
for treating severe RA (DAS28 of more than 5.1) that has inadequately responded
to at least 1 biological DMARD, in people who cannot have rituximab, see the
guidance on:
• filgotinib (TA676, February 2021)
• upadacitinib (TA665, December 2020)
• sarilumab (TA485, November 2017)
• tofacitinib (TA480, October 2017)
• baricitinib (TA466, August 2017)
• certolizumab pegol (TA415, October 2016)
• tocilizumab (TA247, February 2012)
• golimumab (TA225, June 2011)
• abatacept (TA195, August 2010)
• adalimumab (TA195, August 2010)
• etanercept (TA195, August 2010)
• infliximab (TA195, August 2010) .
Give the biological or targeted synthetic DMARD in combination with
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methotrexate unless it is contraindicated, or the person cannot tolerate it.
Abatacept, golimumab, infliximab and tocilizumab are not recommended for
monotherapy.
For abatacept, adalimumab, certolizumab pegol, etanercept, golimumab,
infliximab and tocilizumab, previous biological DMARD treatment should
include at least 1 TNF inhibitor.
1.5.6
For medicines recommended as options in NICE technology appraisal guidance
for treating severe RA (DAS28 of more than 5.1) that has inadequately responded
to at least 1 biological DMARD and rituximab, see the guidance on:
• filgotinib (TA676, February 2021)
• upadacitinib (TA665, December 2020)
• sarilumab (TA485, November 2017)
• tocilizumab (TA247, February 2012) .
Give the biological or targeted synthetic DMARD in combination with
methotrexate unless it is contraindicated, or the person cannot tolerate it.
Sarilumab and tocilizumab are not recommended for monotherapy.
For tocilizumab, previous biological DMARD treatment should include at least
1 TNF inhibitor.
Anakinra
1.5.7
On the balance of its clinical benefits and cost effectiveness, anakinra is not
recommended for the treatment of RA, except in the context of a controlled,
long-term clinical study.
1.5.8
Do not offer the combination of TNF inhibitor therapy and anakinra for RA.
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Glucocorticoids
1.5.9
Offer short-term treatment with glucocorticoids for managing flares in adults with
recent-onset or established disease to rapidly decrease inflammation.
1.5.10
In adults with established RA, only continue long-term treatment with
glucocorticoids when:
• the long-term complications of glucocorticoid therapy have been fully
discussed, and
• all other treatment options (including biological and targeted synthetic
DMARDs) have been offered.
See recommendations on managing glucocorticoid withdrawal in NICE's
guideline on adrenal insufficiency . [2009, amended 2018]
1.6 Symptom control
1.6.1
Consider oral non-steroidal anti-inflammatory drugs (NSAIDs, including traditional
NSAIDs and cox II selective inhibitors), when control of pain or stiffness is
inadequate. Take account of potential gastrointestinal, liver and cardio-renal
toxicity, and the person's risk factors, including age and pregnancy.
1.6.2
When treating symptoms of RA with oral NSAIDs:
• offer the lowest effective dose for the shortest possible time
• offer a proton pump inhibitor (PPI), and
• review risk factors for adverse events regularly.
1.6.3
If a person with RA needs to take low-dose aspirin, healthcare professionals
should consider other treatments before adding an NSAID (with a PPI) if pain
relief is ineffective or insufficient. [2009, amended 2018]
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For a short explanation of why the committee made the 2018 recommendations and
how they might affect practice, see the rationale and impact section on symptom
control .
Full details of the evidence and the committee's discussion are in evidence review G:
Analgesics .
1.7 The multidisciplinary team
1.7.1
Adults with RA should have ongoing access to a multidisciplinary team. This
should provide the opportunity for periodic assessments (see 1.9.2 and 1.9.3) of
the effect of the disease on their lives (such as pain, fatigue, everyday activities,
mobility, ability to work or take part in social or leisure activities, quality of life,
mood, impact on sexual relationships) and help to manage the condition.
1.7.2
Adults with RA should have access to a named member of the multidisciplinary
team (for example, the specialist nurse) who is responsible for coordinating their
care.
1.8 Non-pharmacological management
Physiotherapy
1.8.1
Adults with RA should have access to specialist physiotherapy, with periodic
review (see 1.9.2 and 1.9.3), to:
• improve general fitness and encourage regular exercise
• learn exercises for enhancing joint flexibility, muscle strength and managing
other functional impairments
• learn about the short-term pain relief provided by methods such as
transcutaneous electrical nerve stimulators (TENS) and wax baths.
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Occupational therapy
1.8.2
Adults with RA should have access to specialist occupational therapy, with
periodic review (see 1.9.2 and 1.9.3), if they have:
• difficulties with any of their everyday activities, or
• problems with hand function.
Hand exercise programmes
1.8.3
Consider a tailored strengthening and stretching hand exercise programme for
adults with RA with pain and dysfunction of the hands or wrists if:
• they are not on a drug regimen for RA, or
• they have been on a stable drug regimen for RA for at least 3 months.
1.8.4
The tailored hand exercise programme for adults with RA should be delivered by
a practitioner with training and skills in this area.
Podiatry
1.8.5
All adults with RA and foot problems should have access to a podiatrist for
assessment and periodic review of their foot health needs (see 1.9.2 and 1.9.3).
1.8.6
Functional insoles and therapeutic footwear should be available for all adults with
RA if indicated.
Psychological interventions
1.8.7
Offer psychological interventions (for example, relaxation, stress management
and cognitive coping skills [such as managing negative thinking]) to help adults
with RA adjust to living with their condition.
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NICE has published a guideline on depression in adults with a chronic physical health
problem .
Diet and complementary therapies
1.8.8
Inform adults with RA who wish to experiment with their diet that there is no
strong evidence that their arthritis will benefit. However, they could be
encouraged to follow the principles of a Mediterranean diet (more bread, fruit,
vegetables and fish; less meat; and replace butter and cheese with products
based on vegetable and plant oils).
1.8.9
Inform adults with RA who wish to try complementary therapies that although
some may provide short-term symptomatic benefit, there is little or no evidence
for their long-term efficacy.
1.8.10
If an adult with RA decides to try complementary therapies, advise them:
• these approaches should not replace conventional treatment
• this should not prejudice the attitudes of members of the multidisciplinary
team, or affect the care offered.
1.9 Monitoring
1.9.1
Ensure that all adults with RA have:
• rapid access to specialist care for flares
• information about when and how to access specialist care, and
• ongoing drug monitoring.
1.9.2
Consider a review appointment to take place 6 months after achieving treatment
target (remission or low disease activity) to ensure that the target has been
maintained.
1.9.3
For adults with RA who are receiving a biological or targeted synthetic DMARD,
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continue treatment only if there is a moderate response (as defined in the
relevant NICE technology appraisal guidance listed in section 1.5 ) at 6 months.
Stop treatment if this is not maintained.
1.9.4
Offer all adults with RA, including those who have achieved the treatment target,
an annual review to:
• assess disease activity and damage, and measure functional ability (using,
for example, the Health Assessment Questionnaire [HAQ])
• check for the development of comorbidities, such as hypertension, ischaemic
heart disease, osteoporosis and depression
• assess symptoms that suggest complications, such as vasculitis and disease
of the cervical spine, lung or eyes
• organise appropriate cross referral within the multidisciplinary team
• assess the need for referral for surgery (see section 1.10)
• assess the effect the disease is having on a person's life.
Follow recommendation 1.2.1 if the target is not maintained. [2009, amended
2020]
1.9.5
For adults who have maintained the treatment target (remission or low disease
activity) for at least 1 year without glucocorticoids, consider cautiously reducing
drug doses or stopping drugs in a step-down strategy . Return promptly to the
previous DMARD regimen if the treatment target is no longer met. See
recommendations on managing glucocorticoid withdrawal in NICE's guideline on
adrenal insufficiency .
1.9.6
Do not use ultrasound for routine monitoring of disease activity in adults with RA.
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For a short explanation of why the committee made the 2018 recommendations and
how they might affect practice, see the rationale and impact section on monitoring .
Full details of the evidence and the committee's discussion are in evidence review E:
Frequency of monitoring .
1.10 Timing and referral for surgery
1.10.1
Offer to refer adults with RA for an early specialist surgical opinion if any of the
following do not respond to optimal non-surgical management:
• persistent pain due to joint damage or other identifiable soft tissue cause
• worsening joint function
• progressive deformity
• persistent localised synovitis.
1.10.2
Offer to refer adults with any of the following complications for a specialist
surgical opinion before damage or deformity becomes irreversible:
• imminent or actual tendon rupture
• nerve compression (for example, carpal tunnel syndrome)
• stress fracture.
1.10.3
When surgery is offered to adults with RA, explain that the main expected
benefits are:
• pain relief
• improvement, or prevention of further deterioration, of joint function, and
• prevention of deformity.
Cosmetic improvements should not be the dominant concern.
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Page 19 of 39 1.10.4
Offer urgent combined medical and surgical management to adults with RA who
have suspected or proven septic arthritis (especially in a prosthetic joint).
1.10.5
If an adult with RA develops any symptoms or signs that suggest cervical
myelopathy (for example, paraesthesia, weakness, unsteadiness, reduced power,
extensor plantars):
• request an urgent MRI scan, and
• refer for a specialist surgical opinion.
1.10.6
Do not let concerns about the long-term durability of prosthetic joints influence
decisions to offer joint replacements to younger adults with RA.
Terms used in this guideline
Bridging treatment
Glucocorticoids used for a short period of time when a person is starting a new DMARD,
intended to improve symptoms while waiting for the new DMARD to take effect (which can
take 2 to 3 months).
Conventional disease-modifying anti-rheumatic drugs
(cDMARDs)
Conventional disease-modifying anti-rheumatic drugs are synthetic drugs that modify
disease rather than just alleviating symptoms. They include methotrexate, sulfasalazine,
leflunomide and hydroxychloroquine, but do not include biological DMARDs and targeted
synthetic DMARDs.
Janus kinase (JAK) inhibitor
A targeted synthetic DMARD that inhibits the inflammatory activity of the Janus kinase
enzymes. They are given orally. Examples include baricitinib, filgotinib, tofacitinib and
upadacitinib.
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Palindromic
Palindromic rheumatism is an inflammatory arthritis that causes attacks of joint pain and
swelling similar to RA. Between attacks the joints return to normal.
Step-up strategy
Additional DMARDs are added to DMARD monotherapy when disease is not adequately
controlled.
Step-down strategy
During treatment with 2 or more DMARDs, tapering and stopping at least 1 drug once
disease is adequately controlled.
Synovitis
Soft tissue joint swelling.
Treat-to-target
A treat-to-target strategy is a strategy that defines a treatment target (such as remission
or low disease activity) and applies tight control (for example, monthly visits and
respective treatment adjustment) to reach this target. The treatment strategy often follows
a protocol for treatment adaptations depending on the disease activity level and degree of
response to treatment.
Tumour necrosis factor (TNF) inhibitor
A biological DMARD that inhibits an inflammatory protein, tumour necrosis factor-alpha.
They are given by injection or infusion. Examples include adalimumab, certolizumab pegol,
etanercept, golimumab, and infliximab.
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Recommendations for research
The guideline committee has made the following high-priority recommendations for
research.
Key recommendations for research
1 Analgesics
What is the clinical and cost effectiveness of analgesic drugs other than non-steroidal
anti-inflammatory drugs (NSAIDs) in adults with rheumatoid arthritis (RA) whose pain or
stiffness control is not adequate?
Why this is important
Analgesics (including NSAIDs, paracetamol, opioids and compound analgesics) are
sometimes used with disease-modifying treatments to relieve pain and stiffness when
symptom control is inadequate. Current practice regarding the choice of analgesic in RA is
variable. The evidence is limited for many of the analgesic drugs other than NSAIDs, and
their relative effectiveness is unknown. Further research in this area may inform future
guidance on the use of analgesic drugs other than NSAIDs for controlling symptoms.
2 Short-term bridging treatment with glucocorticoids
What is the clinical and cost effectiveness of short-term bridging treatment with
glucocorticoids for adults with RA starting a new disease-modifying anti-rheumatic drug
(DMARD), including the most effective dosing strategy and mode of administration?
Why this is important
All DMARDs have a slow onset of action. In some cases, response may not be seen for 2 to
3 months. In contrast, glucocorticoids have an immediate effect on joint pain and swelling.
In clinical practice, several different regimens are prescribed to 'bridge' the time between
the initial prescription of DMARDs and the clinical response. However, good quality
evidence from randomised controlled trials (RCTs) demonstrating the effectiveness of
Rheumatoid arthritis in adults: management (NG100)
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glucocorticoids as bridging treatment is limited and inconclusive. Further research is
needed to inform recommendations for practice regarding whether bridging treatment
with steroids should be used until the new DMARD begins to take effect.
The optimal dosing strategy and mode of administration for bridging glucocorticoids also
needs to be established. Although the anti-inflammatory response is dose dependent, side
effects of glucocorticoids vary according to both the dose and the duration of treatment.
For a short explanation of why the committee made the recommendation for research,
see the rationale section on short-term bridging treatment with glucocorticoids .
Full details of the evidence and the committee's discussion are in evidence review H:
Glucocorticoids .
3 Ultrasound in monitoring
What is the clinical and cost effectiveness of using ultrasound to monitor disease in adults
with RA when clinical examination is inconclusive or inconsistent with other signs of
disease activity?
Why this is important
RA is a chronic inflammatory condition that needs regular review to enable adjustments in
management to achieve a target of remission or low disease activity.
Although ultrasound is able to show subclinical inflammation or erosions in some people in
clinical remission, evidence from RCTs does not support using ultrasound for routine
monitoring. However, ultrasound may be useful for assessing disease activity in some
people with RA; specifically, when clinical examination is inconclusive or is inconsistent
with other signs of disease activity (for example, pain or markers of inflammation). There is
no reliable evidence on the added value of ultrasound as part of a monitoring strategy in
these subgroups.
In addition, when there is inconsistency between clinical examination and disease activity,
it may be unclear if the person has subclinical inflammatory synovitis or more of a
widespread pain syndrome, which is not inflammatory. These need very different
treatments, so it is important to define them accurately.
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For a short explanation of why the committee made the recommendation for research,
see the rationale section on monitoring .
Full details of the evidence and the committee's discussion are in evidence review E:
Frequency of monitoring .
4 Ultrasound in diagnosis
What is the clinical and cost effectiveness of using ultrasound in addition to clinical
assessment when there is uncertainty about the diagnosis in adults with suspected RA?
Why this is important
Early diagnosis of RA is essential to reduce the impact of the disease on multiple systems
in the body. The course of RA and the initial presentation can be highly variable; most
people with RA have definite synovitis on clinical assessment, but sometimes this is not
obvious, leading to uncertainty about the diagnosis. Ultrasound is a non-invasive and
relatively inexpensive imaging modality that can detect subclinical synovitis and early
erosive disease. It might help determine an early diagnosis of RA when the diagnosis
would otherwise be uncertain. Early diagnosis enables earlier treatment, providing an
opportunity to improve the longer term outcomes for people with RA. The use of
ultrasound may also allow healthcare professionals to be more confident about ruling out a
diagnosis of RA.
5 Management of poor prognosis
What is the clinical and cost effectiveness of managing RA with a poor prognosis
(identified as presence of anti-cyclic citrullinated peptide [CCP] antibodies or evidence of
erosions on X-ray at diagnosis) with a different strategy from that used for standard
management of RA?
Why this is important
Current recommendations suggest all people with RA should be offered the same
management; however clinical experience suggests that the condition responds less well
in some people and some suffer progressive radiographic damage and impaired function
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despite standard management. Several factors have been identified in the literature that, if
present and identified early in the course of the disease, may predict a poor prognosis
(greater radiographic progression). These include anti-CCP antibody positivity and the
presence of radiographic erosions at baseline. At present it is unclear whether people with
poor prognostic markers should have different management early in the disease, and
whether this would improve radiographic and functional (HAQ) outcomes in this group.
Other recommendations for research
6 Subcutaneous methotrexate
What is the clinical and cost effectiveness of subcutaneous methotrexate compared with
oral methotrexate for adults with early onset RA starting a new DMARD?
Why this is important
Methotrexate is an important drug in the treatment of RA. Subcutaneous administration is
an alternative option for people who have side effects with oral treatment. Evidence on the
effectiveness of subcutaneous methotrexate is lacking, but its effects may be superior,
due to increased bioavailability, and fewer side effects than with oral drugs. Research on
subcutaneous methotrexate will inform future guideline recommendations.
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Rationale and impact
These sections briefly explain why the committee made the recommendations and how
they might affect practice. They link to details of the evidence and a full description of the
committee's discussion.
Investigations following diagnosis
Recommendations 1.1.5 and 1.1.6
Why the committee made the recommendations
Evidence showed that anti-cyclic citrullinated peptide (CCP) antibodies and radiographic
damage at baseline were both important prognostic factors for subsequent radiographic
progression. Anti-CCP antibodies are usually measured and X-rays often taken as part of
diagnosis. When this has not been done, the committee agreed that the tests should be
performed as soon as possible. The results will inform discussions with the patient about
how their rheumatoid arthritis (RA) might progress and reinforce the importance of active
monitoring and rapidly seeking specialist care if the disease worsens.
There was limited evidence on poor function, as measured by the Health Assessment
Questionnaire (HAQ), as a prognostic factor. However, the committee agreed that
functional ability (measured, for example, by HAQ) should be determined at diagnosis to
provide a baseline for assessing response to treatment at the annual review.
Evidence suggests that all people with RA should be offered the same management
strategy; however, in the committee's experience some people may respond less well and
have more progressive radiographic damage and impaired function. Because the evidence
was limited as to whether people with poor prognostic markers should follow a different
management strategy to improve radiographic and functional (HAQ) outcomes, the
committee agreed to make a recommendation for research .
How the recommendations might affect practice
Anti-CCP antibodies are usually measured so there should be no change in current
practice. X-raying the hands and feet and measuring functional ability at baseline reflects
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Page 26 of 39
current best practice, but not everyone with RA currently has these investigations. There
may be an increase in the number of X-rays, especially in units without early inflammatory
arthritis clinics, but this is unlikely to have a substantial resource impact.
Measuring functional ability at baseline will involve a change of practice for some
providers, but the cost is low and so this is not expected to have a substantial resource
impact.
Full details of the evidence and the committee's discussion are in evidence review B: Risk
factors .
Return to recommendations
Investigations (ultrasound in diagnosis)
Why the committee made the research recommendation on
ultrasound in diagnosis
Ultrasound is not used widely in diagnosing RA, but use is increasing and depends on the
clinic and the rheumatologist. Evidence was inconsistent and too limited for the committee
to make any recommendation for or against its use in diagnosis. The committee noted that
the studies generally included only people with clinically definite synovitis and agreed that
ultrasound may be more useful when there is uncertainty about the diagnosis after clinical
assessment. They decided to make a recommendation for research to inform future
guidance on who (if anyone) should have ultrasound to aid diagnosis.
Full details of the evidence and the committee's discussion are in evidence review A:
Ultrasound for diagnosis .
Return to the recommendation for research
Treat-to-target strategy
Recommendations 1.2.1 to 1.2.3
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Why the committee made the recommendations
Strategy and treatment target
Evidence showed that a treat-to-target strategy was more effective than usual care for
managing RA and improved outcomes at no additional cost. The committee agreed that
this approach was more likely to achieve rapid and sustained disease control.
No evidence was identified to indicate whether a target of remission or low disease
activity was more effective. However, the committee agreed that remission (for example, a
DAS28 score of less than 2.6) is the most appropriate target for most people, but for some
who are unable to achieve remission despite a treat-to-target approach with appropriate
escalation, low disease activity (for example, a DAS28 score of less than 3.2) is
acceptable. It was agreed that for those identified as being at risk of poor prognosis, a
target of remission may be more appropriate.
Frequency of monitoring for active disease
No studies were identified that compared different frequencies of monitoring specifically in
people with active disease. The committee noted that the 2009 guideline recommended
monthly monitoring and that this was used in some of the studies of a treat-to-target
strategy. The committee agreed that monthly monitoring of C-reactive protein (CRP) and
disease activity was most appropriate for active disease. This allows dose escalation of
disease-modifying anti-rheumatic drugs (DMARDs), checking the need for short-term
bridging treatment with glucocorticoids and whether people are tolerating the drug
regimen, assessing side effects, providing support and encouraging adherence.
People at risk of poor outcomes
There was no evidence that people with a poor prognosis should have different
management in terms of the treatment target or the frequency of monitoring. However, in
the committee's experience RA often responds less well to standard management in this
group. The committee agreed that the recommendations on treat-to-target with monthly
monitoring should ensure that people with a poor prognosis receive effective treatment,
but they decided to make a recommendation for research to inform future guidance for
managing RA in this group.
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How the recommendations might affect practice
A treat-to-target strategy is current best practice in most NHS settings. The 2016 National
Clinical Audit for Rheumatoid Arthritis and Early Inflammatory Arthritis indicated that
healthcare professionals set a treatment target for about 90% of their patients. Although
the 2018 recommendation specifies a target of remission or low disease activity, rather
than a disease level previously agreed with the person, the committee agreed that these
are the targets commonly used and so this is unlikely to involve a significant change in
practice.
Monthly monitoring was recommended in the 2009 guideline, but the committee
acknowledged that many clinics do not monitor active disease this often. A regional survey
(Tugnet 2013) reported that about two-thirds of people with RA received monthly CRP
monitoring but only a quarter had monthly monitoring of disease activity (with about 40%
in dedicated early arthritis clinics) until disease control was achieved. The committee were
unsure whether these rates reflected practice across England and noted that practice had
improved since the survey was conducted in 2011. However, the committee agreed that
monthly monitoring would likely involve a change in practice in some clinics.
Full details of the evidence and the committee's discussion are in evidence review C:
Treat-to-target .
Return to the recommendations
DMARDs
Recommendations 1.4.1 and 1.4.3
Why the committee made the recommendations
First-line treatment
Evidence showed that starting treatment with more than 1 conventional DMARD (cDMARD)
was no more effective than starting with a single cDMARD. The committee agreed that
cDMARD monotherapy might have fewer side effects and recommended cDMARD
monotherapy as first-line treatment. This differed from the 2009 guideline which
recommended combination therapy. The difference is largely a result of inclusion of
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different evidence and a different approach to analysing that evidence.
Many of the studies included in the 2009 guideline used cDMARDs that are no longer
commonly used in UK practice (for example, ciclosporin), and these studies were excluded
from the evidence for the 2018 update. In addition, the 2018 update included new
evidence published after the 2009 guideline. Further, a different approach to analysing the
evidence was taken, with the 2018 update aiming to identify the most effective cDMARD
strategy (monotherapy, sequential monotherapy, step-up therapy, step-down therapy or
parallel combination therapy) as well as which cDMARD should be used. The 2009
guideline compared treatment strategies only, regardless of the particular cDMARDs, and
combined evidence according to treatment strategy.
The evidence included in the 2018 update was therefore different to that included in 2009
and supported cDMARD monotherapy as first-line treatment.
Evidence from randomised controlled trials (RCTs) in people who had never had a DMARD
showed no consistent differences in the effectiveness of methotrexate, leflunomide and
sulfasalazine as monotherapies. The drugs also had similar costs. The committee agreed
that any of these drugs can be used as first-line treatment.
Hydroxychloroquine was less effective, but fewer people stopped treatment because of
side effects. The committee agreed that hydroxychloroquine could be considered for
people with mild or palindromic disease.
People at risk of poor outcomes
Evidence for different first-line treatment in people with a poor prognosis was limited so
the committee decided not to make a separate recommendation for this group. They
agreed that the recommendation for dose increases and treating to target (with the aim of
keeping disease activity low) should ensure adequate treatment for these people. Given
the limited evidence in this area, the committee also decided that the possible benefit of
managing RA with a poor prognosis with a different strategy was a priority for future
research.
Further treatment
Evidence supported adding another cDMARD when needed (step-up strategy) rather than
replacing the cDMARD with another (sequential monotherapy). The committee
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acknowledged that more side effects were possible with a step-up strategy, but in their
experience these could be managed by drug monitoring and were outweighed by the
clinical benefit of combination treatment when monotherapy was inadequate. A published
economic analysis supported a step-up approach rather than sequential monotherapy.
Subcutaneous methotrexate
No evidence was found for subcutaneous methotrexate, but the committee agreed that
the effects may be superior and side effects fewer than with oral cDMARDs. However,
because subcutaneous methotrexate is significantly more expensive than other cDMARD
options, the committee was not able to recommend this without evidence of clinical
benefit and cost effectiveness relative to oral cDMARDs. The committee decided to make
a research recommendation to inform future guidance.
How the recommendations might affect practice
The 2009 guideline recommended a combination of cDMARDs (including methotrexate
and at least 1 other cDMARD) for newly diagnosed RA and emphasised the importance of
starting effective cDMARD therapy as soon as possible.
The 2009 recommendation to start with combination therapy was not widely adopted. The
2016 National Clinical Audit for Rheumatoid Arthritis and Early Inflammatory Arthritis
reported that only 46% of people with RA received combination cDMARDs at any time.
Currently there is variation in practice regarding the choice of cDMARD(s) and treatment
strategy, with many healthcare professionals preferring to start with monotherapy and
only use combination therapy when response is inadequate.
The 2018 recommendations to start with monotherapy and add drugs when the response
is inadequate are unlikely to have a substantial impact on practice or resources, as they
align with the current approach taken by many healthcare professionals. However, the
recommendations should result in a more consistent treatment strategy and reduce the
number of people prescribed combination therapy on diagnosis.
The 2009 guideline recommended methotrexate as one of the first drugs used in
combination therapy. The 2018 recommendations do not specify which cDMARD should be
used at any stage of treatment. Again, this will be unlikely to have a significant impact on
practice, and methotrexate is likely to remain one of the most commonly prescribed drugs.
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The recommendations on dose escalation and reduction have not changed substantially
from the 2009 guideline and reflect current clinical practice. The committee clarified that
dose reduction and the use of a step-down strategy should only be considered after a
person has maintained the treatment target for at least 1 year without the use of
glucocorticoids.
Full details of the evidence and the committee's discussion are in evidence review F:
DMARDs .
Return to the recommendations
Short-term bridging treatment with
glucocorticoids
Recommendation 1.4.2
Why the committee made the recommendation
Evidence from RCTs on the use of short-term bridging treatment with glucocorticoids to
relieve symptoms while people are waiting for a new DMARD to take effect was limited.
There was some evidence that fewer people withdrew from the studies due to inefficacy
or adverse events when they were taking glucocorticoids, although there was no evidence
that glucocorticoids were effective in terms of disease activity score, quality of life or
function, as studies did not report these outcomes. In the committee's experience people
with active arthritis may benefit from the anti-inflammatory effects of glucocorticoids.
However, for others with less active disease this additional treatment may not be needed.
The committee agreed that short-term glucocorticoids could be considered on a case-by-
case basis.
Because of the lack of good quality evidence, the committee decided to make a
recommendation for research to determine the effectiveness of short-term glucocorticoids
for adults taking a new DMARD, including the most effective regimen.
How the recommendation might affect practice
Most healthcare professionals offer short-term bridging treatment with glucocorticoids to
adults starting a new DMARD. They can continue to offer this but the recommendation
Rheumatoid arthritis in adults: management (NG100)
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encourages them to consider whether this additional treatment is always needed.
Therefore this is unlikely to result in additional spending for the NHS.
Full details of the evidence and the committee's discussion are in evidence review H:
Glucocorticoids .
Return to the recommendation
Symptom control
Recommendations 1.6.1 and 1.6.2
Why the committee made the recommendations
Evidence suggested that non-steroidal anti-inflammatory drugs (NSAIDs) may offer a small
benefit in relieving symptoms for adults with RA (including pain and stiffness). The
committee agreed that this was likely to outweigh the increase in gastrointestinal adverse
events associated with NSAIDs. To minimise adverse events, the committee agreed that
NSAIDs should be used at the lowest doses and for the shortest possible time, with a
proton pump inhibitor, and that risk factors for adverse events should be reviewed
regularly. The recommendations for analgesic treatment in this guideline replace those in
the 2009 guideline.
There was limited evidence on paracetamol, opioids and tricyclic antidepressants and no
evidence for nefopam, gabapentinoids or selective serotonin reuptake inhibitor (SSRI) and
SSNRI antidepressants. The committee acknowledged that the 2009 guideline had
recommended analgesics other than NSAIDs for pain control. However, the 2009 guideline
indicated that the evidence on analgesia other than NSAIDs was 'sparse'. No further
evidence on these drugs was identified since the publication of the 2009 guideline. The
committee for the 2018 guideline decided to make a research recommendation rather than
a practice recommendation on analgesia other than NSAIDs.
How the recommendations might affect practice
Current practice regarding the choice of analgesic is variable, with paracetamol,
compound analgesics and NSAIDs all commonly used to control symptoms. Choice of
analgesic tends to be based on individual effectiveness as well as the person's risk profile,
Rheumatoid arthritis in adults: management (NG100)
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tolerance, and side effects. In particular, there are some groups of people for whom
NSAIDs are unsuitable because of contraindications, comorbidities or tolerability, and
other people who are currently benefiting from analgesic drugs other than NSAIDs. The
current approach is likely to continue but there may be an increase in prescribing of
NSAIDs instead of other analgesic drugs for people with newly diagnosed RA.
Full details of the evidence and the committee's discussion are in evidence review G:
Analgesics .
Return to the recommendations
Monitoring
Recommendations 1.9.1, 1.9.2, 1.9.5 and 1.9.6
Why the committee made the recommendations
Frequency of monitoring when treatment target has been achieved
No evidence was identified on monitoring frequency once the treatment target has been
achieved. However, the committee agreed that once people with RA had achieved the
treatment target, and this was sustained at a 6-month follow-up appointment, there was
no need for additional routine appointments to be scheduled other than the annual review.
All people with RA should have an annual review.
In people with established RA (RA for at least 2 years), the evidence suggested that
patient-initiated rapid access and scheduled medical review every 3 to 6 months were
similarly effective. The committee agreed that all adults with RA should have rapid access
to specialist care for disease flares, and ongoing drug monitoring.
Ultrasound in monitoring
Randomised controlled evidence did not support using ultrasound for routine monitoring of
RA. However, in the committee's experience ultrasound can be useful for monitoring when
clinical examination is inconclusive or is inconsistent with other signs of disease activity
(for example, pain or markers of inflammation). The committee decided to make a
recommendation for research to inform future guidance about using ultrasound in these
Rheumatoid arthritis in adults: management (NG100)
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Page 34 of 39
situations.
How the recommendations might affect practice
The frequency of monitoring and review appointments for people who have reached the
treatment target vary around the country, with some people being seen more often than
needed and others not receiving adequate follow-up. The 2018 recommendations are
likely to reduce unwarranted variation.
Most people with RA currently have rapid access to specialist care when they have a flare.
The 2016 National Clinical Audit for Rheumatoid Arthritis and Early Inflammatory Arthritis
reported that 92% of people had access to urgent advice, with 97% of providers running a
telephone advice line. Therefore the recommendation will not affect current practice.
Use and availability of ultrasound varies widely across the country and even between
healthcare professionals in the same department. Some healthcare professionals use it
routinely whereas others use it on a case-by-case basis. The recommendation should
reduce the overall use of ultrasound while still allowing its use for selected subgroups.
Full details of the evidence and the committee's discussion are in evidence review E:
Frequency of monitoring .
Return to the recommendations
Rheumatoid arthritis in adults: management (NG100)
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Page 35 of 39
Context
Rheumatoid arthritis (RA) is an inflammatory disease largely affecting synovial joints. It
typically affects the small joints of the hands and the feet, and usually both sides equally
and symmetrically, although any synovial joint can be affected. It is a systemic disease and
so can affect the whole body, including the heart, lungs and eyes.
The incidence of the condition is low, with around 1.5 men and 3.6 women developing RA
per 10,000 people per year. The overall occurrence of RA is 2 to 4 times greater in women
than men. The peak age of incidence in the UK for both men and women is the 70s, but
people of all ages can develop the disease.
Drug management aims to relieve symptoms, as pain relief is the priority for people with
RA, and to modify the disease process. Disease modification slows or stops radiological
progression, which is closely correlated with progressive functional impairment.
RA can result in a wide range of complications for people with the disease, their carers,
the NHS and society in general. The economic impact of this disease includes:
• direct costs to the NHS and associated healthcare support services
• indirect costs to the economy, including the effects of early mortality and lost
productivity
• the personal impact of RA and subsequent complications for people with RA and their
families.
Approximately one-third of people stop work because of the disease within 2 years of
onset, and this increases thereafter. Clearly this disease is costly to the UK economy and
to individuals.
Rheumatoid arthritis in adults: management (NG100)
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Page 36 of 39
Finding more information and committee
details
To find NICE guidance on related topics, including guidance in development, see the NICE
topic page on musculoskeletal conditions .
For full details of the evidence and the guideline committee's discussions, see the
evidence reviews . You can also find information about how the guideline was developed ,
including details of the committee.
NICE has produced tools and resources to help you put this guideline into practice . For
general help and advice on putting our guidelines into practice, see resources to help you
put NICE guidance into practice .
Rheumatoid arthritis in adults: management (NG100)
© NICE 2025. All rights reserved. Subject to Notice of rights (
Page 37 of 39 Update information
October 2020: We amended recommendation 1.2.1 to clarify that multiple disease-
modifying anti-rheumatic drugs can be offered one after the other to achieve treatment
targets. We also added a cross-reference to the recommendation from section 1.5 and
recommendation 1.9.3.
July 2018: We have reviewed the evidence and made new recommendations on
investigations following diagnosis, treat-to-target strategy, initial pharmacological
management, symptom control and monitoring. These recommendations are marked
.
We have also made some changes without an evidence review to:
• clarify when urgent referral is needed
• clarify when measuring anti-cyclic citrullinated peptide antibodies might be
considered for diagnosis
• clarify that X-ray of the hands and feet applies to adults with suspected rheumatoid
arthritis (RA)
• clarify that other treatments rather than analgesics should be considered for people
on low-dose aspirin (analgesics other than NSAIDs are no longer recommended)
• clarify that all adults with RA should have an annual review, including those who have
reached their treatment target.
These recommendations are marked [2009, amended 2018] .
Recommendations marked or last had an evidence review in 2009 or 2015.
In some cases minor changes have been made to the wording to bring the language and
style up to date, without changing the meaning.
Minor changes since publication
November 2024: We added links to relevant technology appraisal guidance in the section
on further pharmacological management . Recommendations marked clarify how to
Rheumatoid arthritis in adults: management (NG100)
© NICE 2025. All rights reserved. Subject to Notice of rights (
Page 38 of 39
use medicines recommended in NICE technology appraisal guidance.
August 2024: We added links to NICE's guideline on adrenal insufficiency.
July 2019: Cost analysis was changed to economic analysis in the rationale for DMARDs.
ISBN: 978-1-4731-3003-6
Rheumatoid arthritis in adults: management (NG100) |
11337 | https://www.reddit.com/r/learnmath/comments/j0ftaj/how_to_compare_a_b_and_a_b/ | How to compare |a + b| and |a| + |b|? : r/learnmath
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<Complex numbers | Modulus/Rules/Fact
Proof
We only show the triangle inequality, for the other statements see exercise. Because of (7) we have for every complex number u{\displaystyle {}u} the estimate Re(u)≤|u|{\displaystyle {}\operatorname {Re} \,{\left(u\right)}\leq \vert {u}\vert }. Therefore,
Re(z w¯)≤|z||w|,{\displaystyle {}\operatorname {Re} \,{\left(z{\overline {w}}\right)}\leq \vert {z}\vert \vert {w}\vert \,,}
and hence
|z+w|2=(z+w)(z¯+w¯)=z z¯+z w¯+w z¯+w w¯=|z|2+2 Re(z w¯)+|w|2≤|z|2+2|z||w|+|w|2=(|z|+|w|)2.{\displaystyle {}{\begin{aligned}\vert {z+w}\vert ^{2}&=(z+w){\left({\overline {z}}+{\overline {w}}\right)}\&=z{\overline {z}}+z{\overline {w}}+w{\overline {z}}+w{\overline {w}}\&=\vert {z}\vert ^{2}+2\operatorname {Re} \,{\left(z{\overline {w}}\right)}+\vert {w}\vert ^{2}\&\leq \vert {z}\vert ^{2}+2\vert {z}\vert \vert {w}\vert +\vert {w}\vert ^{2}\&=(\vert {z}\vert +\vert {w}\vert )^{2}.\end{aligned}}}
By taking the square root, we get the stated estimate.
To fact
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11339 | https://www.legislation.gov.uk/ukpga/2006/46/section/40 | Companies Act 2006
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Companies Act 2006
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UK Public General Acts
2006 c. 46
Part 4
Capacity of company and...
Section 40
Table of Contents
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Explanatory Notes
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Act amendment to earlier affecting provision S.I. 2014/3348, art. 220A by S.I. 2024/1115reg. 4(3)
s. 790EB(1A)(1B) inserted by S.I. 2025/1036reg. 4(a)
s. 790EB(3) inserted by S.I. 2025/1036reg. 4(b)
s. 790EC(1A)(1B) inserted by S.I. 2025/1036reg. 5(a)
s. 790EC(3) inserted by S.I. 2025/1036reg. 5(b)
s. 790ED-790EF inserted by S.I. 2025/1036reg. 6
s. 790LF(4) inserted by S.I. 2025/1036reg. 12(b)
s. 790LG(1A) inserted by S.I. 2025/1036reg. 13(3)
s. 790LH(4)(5) inserted by S.I. 2025/1036reg. 14(4)
s. 1098C(1)(ea) inserted by S.I. 2025/1037Sch. 1para. 2(a)(ii)
s. 1098C(2)(e) inserted by S.I. 2025/1037Sch. 1para. 2(b)(iii)
s. 1098C(4A) inserted by S.I. 2025/1037Sch. 1para. 2(c)
Sch. 2 Pt. 2 Section A para. 25(m)(ii) words omitted by S.I. 2025/381Sch.para. 19
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s. 790EB(1A)(1B) inserted by S.I. 2025/1036reg. 4(a)
s. 790EB(3) inserted by S.I. 2025/1036reg. 4(b)
s. 790EC(1A)(1B) inserted by S.I. 2025/1036reg. 5(a)
s. 790EC(3) inserted by S.I. 2025/1036reg. 5(b)
s. 790ED-790EF inserted by S.I. 2025/1036reg. 6
s. 790LF(4) inserted by S.I. 2025/1036reg. 12(b)
s. 790LG(1A) inserted by S.I. 2025/1036reg. 13(3)
s. 790LH(4)(5) inserted by S.I. 2025/1036reg. 14(4)
s. 1098C(1)(ea) inserted by S.I. 2025/1037Sch. 1para. 2(a)(ii)
s. 1098C(2)(e) inserted by S.I. 2025/1037Sch. 1para. 2(b)(iii)
s. 1098C(4A) inserted by S.I. 2025/1037Sch. 1para. 2(c)
Sch. 2 Pt. 2 Section A para. 25(m)(ii) words omitted by S.I. 2025/381Sch.para. 19
40 Power of directors to bind the company U.K.
This section has no associated Explanatory Notes
(1)In favour of a person dealing with a company in good faith, the power of the directors to bind the company, or authorise others to do so, is deemed to be free of any limitation under the company's constitution.
(2)For this purpose—
(a)a person “deals with” a company if he is a party to any transaction or other act to which the company is a party,
(b)a person dealing with a company—
(i)is not bound to enquire as to any limitation on the powers of the directors to bind the company or authorise others to do so,
(ii)is presumed to have acted in good faith unless the contrary is proved, and
(iii)is not to be regarded as acting in bad faith by reason only of his knowing that an act is beyond the powers of the directors under the company's constitution.
(3)The references above to limitations on the directors' powers under the company's constitution include limitations deriving—
(a)from a resolution of the company or of any class of shareholders, or
(b)from any agreement between the members of the company or of any class of shareholders.
(4)This section does not affect any right of a member of the company to bring proceedings to restrain the doing of an action that is beyond the powers of the directors.
But no such proceedings lie in respect of an act to be done in fulfilment of a legal obligation arising from a previous act of the company.
(5)This section does not affect any liability incurred by the directors, or any other person, by reason of the directors' exceeding their powers.
(6)This section has effect subject to—
section 41 (transactions with directors or their associates), and
section 42 (companies that are charities).
Modifications etc. (not altering text)
C1 S. 40 applied (with modifications) (1.10.2009) by The Unregistered Companies Regulations 2009 (S.I. 2009/2436), regs. 3-5, Sch. 1 para. 3(a) (with transitional provisions and savings in regs. 7, 9, Sch. 2)
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11340 | https://www.math.northwestern.edu/~scanez/courses/320/notes/supinf.pdf | Notes on Supremums and Infimums The purpose of these notes is to elaborate on the notions of supremums and infimums discussed in the book.
The book gives some very basic definitions, but these topics deserve much more attention paid to them. Here we give some further characterizations and properties of these two ideas.
Supremums Definition. The supremum (or least upper bound) of a set S ⊆R which is bounded above is an upper bound b ∈R of S such that b ≤u for any upper bound u of S. We use the notation b = sup S for supremums.
Note that there are two definining properties of sup S: (i) it is an upper bound of S, and (ii) it is smaller than or equal to any other upper bound of S. Both of these are crucial.
The following justifies us talking about the supremum of a set as opposed to a supremum: Proposition. The supremum of a set, if it exists, is unique.
Proof. Suppose that S ⊆R is bounded above and that a, b ∈R are supremums of S. Note that in particular both a and b are then upper bounds of S.
Since a is a least upper bound of S and b is an upper bound of S, a ≤b. Similarly, since b is a least upper bound and a an upper bound of S, b ≤a. Thus a = b, showing that the supremum of a set is unique.
Intuitively, another way of stating the definition of supremum is that no number smaller than the supremum can be an upper bound of the given set. The following makes this precise: Proposition. An upper bound b of a set S ⊆R is the supremum of S if and only if for any ϵ > 0 there exists s ∈S such that b −ϵ < s.
For practice, try to give a precise proof of this, but the intuition is the following. The statement “there exists s ∈S such that b −ϵ < s” means exactly that b −ϵ is not an upper bound of S; in other words, this is the negation of what it means to say that u ∈R is an upper bound of S: for any s ∈S, s ≤u. As ϵ varies over all positive real numbers, b −ϵ varies over all real numbers smaller than b, so the condition given in the proposition precisely says that for an upper bound b of S, b = sup S if and only if no number smaller than b is an upper bound of S.
This next proposition requires material on convergent sequences, which we will discuss in Chap-ter 2: Proposition. Suppose that S ⊆R is bounded above and that b ∈R is an upper bound of S. Then b = sup S if and only if there exists a sequence (xn) of elements in S converging to b.
Proof. Suppose that b = sup S. For any n ∈N, the previous proposition tells us that there exists xn ∈S such that b −1 n < xn.
Since also xn ≤b because b is an upper bound of S, this implies that |xn −b| < 1 n, from which it follows that the sequence (xn) thus obtained converges to b as required.
Conversely, suppose that there is a sequence (xn) of elements of S converging to b. For any ϵ > 0, there exists N ∈N so that |xN −b| < ϵ.
Unwinding this inequality gives −ϵ < xN −b < ϵ, and so in particular b −ϵ < xN. Hence b satisfies the condition in the previous proposition which is equivalent to b being the supremum of S, so b = sup S as claimed.
Infimums All of the above statements have analogs for infimums: Definition. The infimum (or greatest lower bound) of a set S ⊆R which is bounded below is a lower bound a ∈R of S such that ℓ≤a for any lower bound ℓof S. We use the notation a = inf S for infimums.
Proposition. The infimum of a set, if it exists, is unique.
The following says that no number smaller than an infimum can be a lower bound of the given set: Proposition. A lower bound a of a set S ⊆R is the infimum of S if and only if for any ϵ > 0 there exists s ∈S such that s < a + ϵ.
Proposition. Suppose that S ⊆R is bounded below and that a ∈R is a lower bound of S. Then a = inf S if and only if there exists a sequence (xn) of elements in S converging to a.
You should try to prove that above facts for practice. They are similar to the proofs for the corresponding facts about supremums with slight modifications.
Here is useful relationship between the above notions: Proposition. Suppose that S ⊆R is nonempty and bounded above and let −S := {−x | x ∈S}.
Then −S is bounded below and inf(−S) = −sup S.
Proof. First we show that −S is bounded below. Let u be an upper bound of S, so that s ≤u for all s ∈S.
Then −s ≥−u for all s ∈S, so −u is less than or equal to anything in −S. Hence −u is a lower bound of −S, so −S is bounded below.
Now, to show that inf(−S) = −sup S, we show that −sup S satisfies the defining properties of inf(−S). First, since sup S is an upper bound of S, what we just showed above tells us that −sup S is indeed a lower bound of −S. Let ℓ∈R be a lower bound of −S; then ℓ≤−s for all s ∈S.
Multiplying through by −1 gives s ≤−ℓfor all s ∈S, so −ℓis an upper bound of S. Hence sup S ≤−ℓby definition of supremum, so ℓ≤−sup S. Thus −sup S is greater than or equal to any lower bound of −S, so we conclude that −sup S = inf(−S) as claimed.
The moral of the above result is that changing signs exchanges supremums and infimums.
2 Examples Claim. inf (0, ∞) = 0 Proof. Since (0, ∞) consists of all real numbers greater than 0, 0 is a lower bound of (0, ∞). Let ϵ > 0. Then ϵ 2 ∈(0, ∞) and ϵ 2 < 0 + ϵ.
Hence 0 satisifes the alternate characterization of infimums given in one of the propositions, so 0 = inf (0, ∞) as claimed.
Claim. sup 1 −1 n | n ∈N = 1 Thoughts. Let’s call this set S. It should be clear that 1 is an upper bound of S, since 1 minus something positive is always smaller than 1. To show that 1 is the supremum of S, we will use the characterization of supremums given in one of the propositions.
So, given any ϵ > 0, we want to find an element s ∈S such that 1 −ϵ < s. Again, this will say that for any ϵ > 0, 1 −ϵ is not an upper bound S, so nothing smaller than 1 is an upper bound of S and thus 1 must be the least upper bound.
Now, the s we want to find will be of the form s = 1 −1 N for some N ∈N since these is precisely what elements of S looks like. So we want to find something of the form 1 −1 N so that 1 −ϵ < 1 −1 N .
But this inequality is the same as ϵ > 1 N , and this finally tells us how to choose N. All of this is scratch work telling us how to find the element s we need, and now we can give the final proof.
Proof of Claim. First, since 1 n > 0 for all n ∈N, 1 −1 n < 1 for all n ∈N so 1 is an upper bound of the given set. Now, let ϵ > 0. Pick N ∈N such that 1 N < ϵ; such a natural number exists by the Archimedean Property of R. Then −1 N > −ϵ so 1 −ϵ < 1 −1 N .
Since 1 −1 N is an element of the given set, this shows that no number smaller than 1 can be an upper bound of the given set—i.e. 1 satisfies the condition given in the alternate characterization of supremums in one of the propositions. Thus sup 1 −1 n | n ∈N = 1 as claimed.
Claim. Suppose that A and B are subsets of R which are nonempty and bounded below. Then inf (A ∪B) = min{inf A, inf B}.
Proof. Since inf A is a lower bound of A and inf B is a lower bound of B, the smaller of these two is a lower bound of A ∪B. If t ∈R is any lower bound of A ∪B, it is in particular a lower bound of A, so t ≤inf A, and it is a lower bound of B, so t ≤inf B. Hence t ≤min{inf A, inf B}, so we conclude that inf (A ∪B) = min{inf A, inf B} since the latter is a lower bound of A ∪B which is greater than or equal to any other lower bound.
To leave you with something to think about: if in the above situation A ∩B ̸= ∅, so that A ∩B has an infimum, what can we say about inf (A ∩B) in relation to inf a and inf B, if anything?
3 |
11341 | https://radiopaedia.org/articles/epiploic-foramen-1?lang=us | Epiploic foramen | Radiology Reference Article | Radiopaedia.org
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Epiploic foramen
Last revised by Jeremy Jones on 12 Aug 2025
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Citation, DOI, disclosures and article data
Citation:
Jones J, Ismail M, Rizk M, et al. Epiploic foramen. Reference article, Radiopaedia.org (Accessed on 29 Sep 2025)
DOI:
Permalink:
rID:
6059
Article created:
14 Apr 2009, Jeremy Jones
At the time the article was created Jeremy Jones had no recorded disclosures.
View Jeremy Jones's current disclosures
Last revised:
12 Aug 2025, Jeremy Jones
Disclosures: At the time the article was last revised Jeremy Jones had no financial relationships to ineligible companies to disclose.
View Jeremy Jones's current disclosures
Revisions:
16 times, by 14 contributors - see full revision history and disclosures
Systems:
Gastrointestinal
Sections:
Anatomy
Tags:
epiploic foramen, cases
Synonyms:
Foramen of Winslow
More Cases Needed: This article has been tagged with "cases" because it needs some more cases to illustrate it. Read more...
The epiploic foramen, also called the foramen of Winslow, is a small vertical passage between the greater sac(peritoneal cavity proper) and the lesser sac (omental bursa), allowing communication between these two spaces.
The foramen is eloquently described as the opening to the lesser sac located "between the two great veins of the abdomen (portal vein and inferior vena cava)" 3.
Gross anatomy
Boundaries
anterior: the free edge of the lesser omentum (hepatoduodenal ligament) which contains the common bile duct, hepatic artery proper, and portal vein between its two layers
posterior: peritoneum covering the inferior vena cava
superior: peritoneum covering the lower margin of caudate lobe of the liver
inferior: peritoneum covering the commencement of the duodenum (D1) and the hepatic artery proper, the latter passing forward below the foramen before ascending between the two layers of the lesser omentum
Related pathology
lesser sac hernia
Quiz questions
Question 3468
Report problem with question
What is the anatomical communication between the greater and lesser sacs of the peritoneal cavity called?
epiploic foramen
hepatorenal fossa
omental bursa
pouch of Douglas
right paracolic gutter
SubmitSkip question
References
Anatomy of the Human Body. (2000) ISBN: 1587341026 - Google Books
Cimmino C. Lesser Sac Hernia via the Foramen of Winslow; a Case Report. Radiology. 1953;60(1):57-9. doi:10.1148/60.1.57 - Pubmed
Robert M. H. McMinn. Last's Anatomy. (2019) ISBN: 9780729543576 - Google Books
Incoming Links
Articles:
Inferior vena cava
Posterior right subhepatic space
Order of structures in the porta hepatis (mnemonic)
Right subhepatic space
Lesser sac
Abdominal hernia
Lesser sac hernia
Portal vein
Gallbladder
Hepatoduodenal ligament
Cases:
Bile leak demonstrating the foramen of Winslow
Caecal internal hernia through the foramen of Winslow
Internal herniation of caecum into lesser sac
Lesser sac hernia
Multiple choice questions:
Question 3468
Related articles: Anatomy: Abdominopelvic
Anatomy: Abdominopelvic
skeleton of the abdomen and pelvis[+][+]
lumbar spine
bony pelvis
innominate bones
pubis
pubic symphysis
obturator foramen
ischium
greater sciatic notch
lesser sciatic notch
ilium
sacrum
sacral hiatus
sacrotuberous ligament
sacrospinous ligament
greater sciatic foramen
lesser sciatic foramen
coccyx
anterior angulation of the coccyx
muscles of the abdomen and pelvis[+][+]
diaphragm
sternocostal triangle
anterior abdominal wall
Scarpa's fascia
muscles
external oblique muscle
inguinal ligament
lacunar ligament
internal oblique muscle
conjoint tendon
transversus abdominis muscle
rectus abdominis muscle
rectus sheath
linea alba
umbilicus
arcuate line
semilunar line
transversalis fascia
pyramidalis muscle
surface anatomy
posterior abdominal wall
psoas major muscle
psoas minor muscle
quadratus lumborum muscle
iliacus muscle
pelvic floor
levator ani muscle
coccygeus muscle
piriformis muscle
obturator internus muscle
spaces of the abdomen and pelvis
anterior abdominal wall[+][+]
sternocostal triangle
posterior abdominal wall[+][+]
superior lumbar triangle
inferior lumbar triangle
iliopsoas compartment
abdominal cavity
peritoneum
peritoneal ligaments[+][+]
left triangular ligament
right triangular ligament
falciform ligament
umbilical vein
ligamentum teres
veins of Sappey
omentum
hepatogastric ligament
gastrosplenic ligament
splenorenal ligament
mesentery[+][+]
small bowel mesentery
root of the mesentery
mesoappendix
transverse mesocolon
sigmoid mesocolon
peritoneal spaces
supramesocolic space
right supramesocolic space
right subphrenic space
right subhepatic space[+][+]
anterior right subhepatic space
posterior right subhepatic space (Morison pouch)
lesser sac
epiploic foramen (of Winslow)
left supramesocolic space(left perihepatic space)[+][+]
leftsubhepatic space
anterior left subhepatic space
posterior left subhepatic space
left subphrenic space
anterior left subphrenic space
posterior left subphrenic (perisplenic) space
inframesocolic space[+][+]
right inframesocolic space
left inframesocolic space
right paracolic gutter
left paracolic gutter
inguinal canal (mnemonic)
Hesselbach triangle
umbilical folds[+][+]
median umbilical fold
medial umbilical folds
lateral umbilical folds
retroperitoneum[+][+]
perirenal fascia
anterior pararenal space
perirenal space
perinephric bridging septa (of Kunin)
posterior pararenal space
properitoneal fat
great vessel space
lateroconal fascia
pelvic cavity[+][+]
pelvic peritoneal space
rectouterine pouch (pouch of Douglas)
rectovesical pouch
retropubic space (of Retzius)
paravesical space
lateral fossa
supravesical fossa
presacral space
canal of Nuck
pudendal canal
obturator canal
perineum[+][+]
urogenital triangle
superficial perineal pouch
perineal membrane
deep perineal pouch
anal triangle
transverse perineal muscles
deep transverse perineal muscles
superficial transverse perineal muscles
ischioanal fossa
urogenital diaphragm
abdominal and pelvic viscera[+][+]
gastrointestinal tract
esophagus
phrenic ampulla
gastro-esophageal junction
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11342 | https://www.youtube.com/watch?v=Kpz4yDpgicA | Maximization and Minimization Problems on Feasible Regions
Houston Math Prep
51300 subscribers
35 likes
Description
6805 views
Posted: 11 May 2020
This video explains maximization and minimization problems in linear programming. We show you how to maximize and/or minimize an objective function over a feasible region. We work several examples, which include both bounded and unbounded regions, and discuss the effect that each has on the results of finding a maximum or a minimum on the feasible region. Our examples in this video use systems of linear inequalities already graphed in our previous video from this series.
0:00 Intro
1:00 Example 1
3:59 Example 2
8:04 Example 3
12:43 Example 4
16:17 Example 5
Video that shows how to graph each feasible region used in this video:
Houston Math Prep Finite/Business Math Playlist:
Houston Math Prep YouTube:
Transcript:
Intro hey everyone Houston math prep here we want to talk to you in this video about finding maximum and minimum values for some equation over a feasible region so we assume you know how to graph systems of inequalities we're going to be referring back to systems that we graphed and solved already when we maximize or minimize some equation usually it's written as Z equals some number times X plus some number times y when we maximize or minimize an equation like this on a system of linear inequalities that maybe looks something like this where we've graphed the inequalities and found a region as our solution for our system of inequalities we call that graphed region the feasible region so this is the region that is all of the solutions for just the system of inequalities not taking into account this equation yet when we have a maximum and/or a minimum value for this equation on this region it is going to occur at one of the vertices of the region in other words it's going to occur at one of the corner points here let's look at our first Example 1 example so this is our first system of inequalities we did in our system of inequalities video so if we want to maximize Z equal to 4x plus 7 Y on this region then that means that the maximum that we can get for Z using this formula is going to occur at one of these corner points so what we'll need to do with our feasible regions be able to find the vertices find the corner points we'll need to label them and then we'll see which one gives us in this case since we're finding the maximum we're gonna find out which point gives us the most out of this equation so I'm gonna go ahead and just label my vertices you can see all of these are on an axis so it's pretty easy to find this bottom corner of the triangle obviously is at 0 0 it's at the origin so that's one of our points over here my x-intercept is at 5 and so this point here is actually at 5 comma 0 and this other intercept here is actually at 2 on the y axis so this is actually at 0 comma 2 so we have all of these vertices here one of these is going to give us the most out of this equation when we plug it in to find the value so let's figure out which of these is the maximum for this equation on the region so I'm going to plug in is zero-zero I'm going to plug in zero two and I'm going to plug in five comma zero and we'll see which one gives us the most so into this Z equals equation so 4x plus 7y if i plug in zero zero that would be four times zero plus 7 times zero i think that gives us zero or that one if i plug in 0 comma 2 so 0 for X and 2 for Y then that would be 4 times 0 plus 7 times y and my Y is 2 here right so this is 0 and this is 14 so 0 plus 14 gives us 14 for this one if I plug in 5 comma 0 into this then I will get 4 times 5 plus 7 times 0 for my Z and that would be 20 plus 0 is going to give us 20 and so we get Z values of 0 and 14 and 20 and we want to maximize so we choose whichever one is the greatest of these values so this is the highest value I have a maximum of 20 that occurs that occurs at the point 5 comma 0 right so also say at the point 5 comma 0 ok so the idea is this triangle is our feasible region and if I want to find where in this region do I get the most out of the formula for X plus 7 y I plug in all my vertices my corner points see which one gives me the most since I'm looking for the max and that's my answer and that's where it occurs let's Example 2 look at this next one here we want to maximize and minimize so we want to find the point that gives us both the most and the least my formula is Z equals 5x plus 6y and here I have this system that we already solved and graphed in our video right before this in the series I went ahead and labeled which of these lines is which equation in my system here obviously my axes are my x equals 0 and y equals 0 equations here some of the vertices in these feasible regions are going to be easy to find anything that's on an axis should be easy right this is 0 0 that's super easy to find this 6 0 even if I didn't have this labeled maybe quite as well I should have probably been able to find this when I graphed my X plus y equals 6 I probably had already labeled this and sketched this point to draw the line so this 6 comma 0 is something I should probably also already know and this one here at 0 comma 4 I should also probably know that one as well when I graphed my 7 X plus 14 y equals 56 using intercepts I probably already knew what this point was the trick is I think figuring out what is this point here where these cross now you could solve this by hand but I think an efficient way to do this might be to solve this by graphing calculator and what we'll want to be able to do is solve systems by matrices so if we put both of these equations in a matrix and let's say we ref in a matrix both of these so we would ref 7 14 56 along with the row 1 1 6 and then we could figure out what this point is if you're if you're labeled really really well and you know you've plotted this with super straight lines you might be able to tell exactly that this is the point 4 comma 2 but if you're sort of sketching this by hand it might be hard to tell what a vertex is when it's two diagonal lines crossing each other and so one short quick way to do that is to get really good at solving systems using ref with a calculator and doing it with matrices but we've got all our vertices let's write all those down so we have 0 0 we'll plug that in we also have 0 comma 4 we have 6 comma 0 and we have 4 comma 2 and we're going to plug all these in and we're maximizing and minimizing so we'll figure out which one gives us the most and the least if I plug in 0 0 that would be 5 times 0 plus 6 times 0 well that's going to give us 0 right if we plug in 0 comma 4 then we'll have 5 times 0 plus 6 times 4 and that will give us 24 if we plug in 6 comma 0 we would have 5 times 6 now plus 6 times 0 that's 30 plus 0 so that would give us 30 and then plugging in 4 comma 2 we would get 5 times 4 plus 6 times 2 5 times 4 is 20 plus another 12 that would give us 32 so if we look back here and we want the max and the min my biggest value I get out of the formula 5x plus 6 y 32 this is our max right and 0 is our smallest value so that's our men so we would go ahead and say maximum of 32 at the point we plugged in was 4 comma 2 right to get that one so at 4 comma 2 that's our max and then our men are minimum of zero and that happened at the origin right so that's at zero comma zero and that would be our answer for both the max and the min on this feasible region given Z equals 5x plus 6y Example 3 let's look at another example where we maximize and minimize here we have the equation Z equals 4x plus 3y so we're gonna Max and min that on this feasible region we went ahead and did the work of solving this feasible region in our previous systems of inequalities video 8x + 6 y less than equal 144 so we've got this 8x plus 6y equals 144 line here X minus 2 y less than equal negative 4 so I've got labeled here my X minus 2 y equals negative 4 and then X greater than equals 0 X equal to 0 is the y-axis here so those were the boundaries of this this is a bounded region here we already should know some of these intercepts or we could kind of look at the equations and tell the y intercept here is actually at 2 so this is at 0 comma 2 I should also know this intercept since it's on an axis when I graphed this I probably knew that this was at y equal to 24 so that's 0 comma 24 you could always just zero out the X term and solve for y if you want to get that if you haven't already done this with us in the last video and then the big question again becomes what is this point here where the two diagonal lines are meeting so remember we can find that point there by row reducing and doing it quickly in a graphing calculator that uses matrices so setting up the coefficients right we could ref 8 6 144 along with the row 1 negative 2 negative 4 and if we do that we should get that this point is 12 comma 8 okay so we have our three vertices we have 0 24 0 2 and 12 8 let's go ahead and write those down 0 comma 2 0 comma 24 and 12 comma 8 and we'll plug these into the formulas equals 4x plus 3y and see which one gives us the most and the least so this one would say 4 times 0 plus 3 times 2 that's 0 plus 6 that gives us 6 they're plugging in 0 24 we would have 4 times 0 plus 3 times 24 that's 0 plus 72 there so this would be 72 and plugging in 12 comma 8 so we would have 4 times 12 plus 3 times 8 now 4 times 12 is 48 plus 3 times 8 which is 24 48 plus 24 gives us 72 so now an interesting thing happens here right I think you can tell certainly that this is our minimum right so we would certainly say that there is a minimum of six and that occurs at the point we plugged in zero comma two right so at zero comma 2 and now this oddball situation happens here we have a tie right we have two things being the exact same highest value over the region so when we have a tie at two vertices in our feasible region what that's saying is that 0 24 and 12 comma 8 when I plug those in I get the same amount out of this formula and it turns out because this is a linear feasible region every point on the line in between those is also going to be a max of the same value so we would actually say that there is a maximum of 72 apt the point 0:24 and at 12 comma 8 and also all points in between and all points on that line in between those two points so a little bit more to write than usual there but that's our answer for this one so when you have a tie whether it's for a min or a max then both of those points will give you that Max or min so they're considered both to be the max or both to be the min and if we're dealing with a linear region in other words if we have lines for all the boundaries of our region then also every point on the line in between those two vertices is also going to be a max or a min in whatever case you have it so we want to look at Example 4 two more examples these regions are a little bit different our feasible regions here you'll notice I have certainly a corner here at this point and I also have a corner point here so I have those two vertices as well but what happens with our feasible region as we graphed this in our last video systems of linear inequalities this region just keeps going up as long as it stays between these two vertical lines here it just keeps continuing up forever so we get what's called an unbounded region when you have an unbounded region it's possible that you may not have a min or you may not have a max or you may not have both actually we're just going to minimize on this region because this one actually because it keeps going up forever has no maximum based on this formula so we're just going to find the minimum for this one now you'll notice that neither of these vertices are actually an intercept right so I might need to ref both of these to figure out what the points are now what you might do is you might just look at this and say well this one's where x equals two so I'm just going to plug in you know x equals two and I'm going to solve for y manually and that's certainly fine and you know here you could plug in x equals ten into this other one where they meet you could get your vertex that way as well we're just going to go ahead and talk about roughing these and not use algebra to solve by hand so this one here I have 2x plus 5y equals 30 at that corner point so 2 5 30 and what does that mean well that meets the line x equals 2 at that point so that would be 1 0 2 in a matrix now you'll notice one of these is already reduced right so it's only going to reduce this top row and this point here is going to end being two comma five point two we get five point two for our y-value here if we want to ref this one so this line here is certainly where the 2x plus 5y equals 30 meets a line right so we would put two five and thirty in this matrix as well but this line meets the x equals ten line at that point so we would put one zero ten in as our second row again you can solve this by hand if you'd like if we ref this I think you'll figure out that we get the point 10 comma 2 for this one here okay so in this case we only have two vertices to check and then whichever one is less will give us the minimum right so we have two comma five point two and we also have 10 comma 2 okay if we plug 2 comma 5 point 2 into 5x plus 15y then that will give us 5 times 2 plus 15 times 5 point 2 and if we figure out what that is that gives us a total of 88 and our 10 comma 2 if we plug that in that would be 5 times 10 plus 15 times 2 and that gives us 50 plus 30 and so that's 80 so we have 80 and 88 and if I want to minimize then I choose the smaller value so 80 is going to be our minimum there so we would say a minimum of 80 we'll say that it occurs at the point 10 comma 2 Example 5 okay let's look at one more with an unbounded region so here I have my last unbounded region from our previous video here's our system we were in the first quadrant and we also had to be above both of these diagonal lines here and I've labeled which they are we want to minimize Z equals 20x plus 12y on this region this region is unbounded it's going up and to the right the shading continues up and right forever so this is an unbounded region so it is possible that this doesn't have a min or a max or both but because it's going up and to the right forever and based on my equation here this actually doesn't have a max you will find but we're going to find the min because there is actually a min that we can find so let's go ahead and figure out where our vertices are so a couple of these are on an axis so when you graph two these lines and set up your region you probably figured these out or you could easily now so this is the point 0 comma 12 y-intercept of 12 and this is an x-intercept of 10 so that point there is 10 comma 0 and the only thing left to find is this point where the two diagonal lines intersect right so to solve this we could go ahead and ref this and so one of my equations is 10 5 60 as a row in the matrix and the other one would be to 520 as a row in the matrix and so we could go ahead and ref that and I think we'll see and that this turns out to be the point 5 comma 2 so our vertices are just 0 12 and 10 0 and 5 2 we will plug those into our formula we're trying to minimize so here I would have 20 X would be 20 times zero plus 12 y would be 12 times 12 that's zero plus 144 that'll be a hundred and forty-four for this one ten comma zero I have 20 X would be 20 times 10 plus 12 y would be 12 times zero in this one 20 times 10 is going to give us 200 there and then 5 comma 2 that will give us 20 times 5 4 20 X + 4 12 y that will give us 12 times 2 and 20 times 5 is a hundred plus 24 so we get a hundred and twenty-four there so I look at 144 200 and 124 and I want the minimum so I would choose this as my minimum since it's the smallest output so we would say here we have a minimum of 124 and it occurs at the point we plugged in 5 comma 2 to get that minimum so at 5 comma 2 in other words when X is 5 and when y is 2 okay everyone hopefully this gives you a good idea of how to find a max or a min or both on your feasible regions remember to decide if you have an unbounded or a bounded region if you have a bounded region you're guaranteed to have a Max and a min on that region if you have an unbounded region just remember you may not have one or you may not have both of them thanks for watching we'll see you in the next video |
11343 | https://math.stackexchange.com/questions/2881759/substitution-in-functional-equation | Stack Exchange Network
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Substitution in functional equation
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When solving functional equations it can be helpful to substitute another function, say, g(x) rather than x to the original functional equation h(x). Under what condition is this a permissible substitution that leaves the original solution intact? Is bijectivity sufficient and if so, why is it?
Example: h(1-h(x))=x. Can I substitute g(x) for x in this equation?
functional-equations
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edited Aug 13, 2018 at 21:47
TaylorJamesTaylorJames
asked Aug 13, 2018 at 20:06
TaylorJamesTaylorJames
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$\begingroup$ Welcome to MSE. Please give some context (see Get answers to practical, detailed questions). $\endgroup$
user539887
– user539887
2018-08-13 20:15:34 +00:00
Commented Aug 13, 2018 at 20:15
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Any substitution is possible whenever the necessary assumptions are fulfilled. They are often helpful to simplify the equation in question. Let $h\colon\Bbb R\to\Bbb R$. Put $1-h(x)$ instead of $x$. Hence $h(1-x)=1-h(x)$, so $$h(x)+h(1-x)=1,$$ which, maybe, maynot, allows us to gain some extra properties of the solution. For instance, for $x=\frac{1}{2}$ we get $h\bigl(\frac{1}{2}\bigr)=\frac{1}{2}.$ This is not so visible by the original equation.
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edited Aug 13, 2018 at 22:41
answered Aug 13, 2018 at 22:28
szw1710szw1710
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$\begingroup$ Thank you. But is h(x) + h(1-x) = 1 equivalent to the original equaition and if so, why is it? Because then I could make further elaboartions on the newly derived expression without losing information. $\endgroup$
TaylorJames
– TaylorJames
2018-08-13 22:51:17 +00:00
Commented Aug 13, 2018 at 22:51
$\begingroup$ I assumed that $h$ is a solution. This is an implication only. For example, the identity map fulfils the equation of mine, but this is not a solution of the original equation. Nevertheless, the addditional knowledge of a solution could be derived from here. This is a necessary condition. If you collect enough information, you could check whether or not the function you arrived at is a solution of the original equation. $\endgroup$
szw1710
– szw1710
2018-08-13 22:53:03 +00:00
Commented Aug 13, 2018 at 22:53
$\begingroup$ Does this mean that any solution of the original function must also satisfy your function? And why is this? $\endgroup$
TaylorJames
– TaylorJames
2018-08-13 23:00:18 +00:00
Commented Aug 13, 2018 at 23:00
$\begingroup$ Does this mean that all solutions to the original function must satisfy your function? I must determine the values of the sum = f(-100) + f(-99) ... + f(100) + f(101) for all possible f which would lead to all sums being equal to 101 as the rest would cancel out $\endgroup$
TaylorJames
– TaylorJames
2018-08-13 23:09:21 +00:00
Commented Aug 13, 2018 at 23:09
$\begingroup$ The first question is whether there exists a function satisfying the original equation. Next, if we suppose there is such function, you are right, with my equation (implied by the original one) your task is trivial. Now we have what follows: if $f$ fulfils the original equation, then the sum in question is $101$. $\endgroup$
szw1710
– szw1710
2018-08-14 00:59:10 +00:00
Commented Aug 14, 2018 at 0:59
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How do you prove ∑n k=1 e 2 π k i n=0∑k=1 n e 2 π k i n=0 for the positive integer n?
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Alon Amit
PhD in Mathematics; Mathcircler. · Upvoted by
Richard Zhou
, B.S./M.S. Mathematics, Yale University (2022) and
Fabio García
, MSc Mathematics, CIMAT (2018) · Author has 8.7K answers and 172M answer views
·Updated 6y
Originally Answered: How do you prove \displaystyle\sum_{k=1}^ne^{\frac{2\pi ki}{n}}=0 for the positive integer n? ·
Up to you. Do you like symmetry? Algebraic symmetry? Geometric symmetry? Polynomials? Fields? There are lots of ways to see this, all valuable.
If you recognize these numbers as the roots of unity of order n n, you can look at answers for this older question.
Let’s suppose you don’t. You don’t know anything about roots of unity or the geometry of complex numbers. But you do know something. You know that a b a c=a b+c a b a c=a b+c, and you know that e 2 π i=1 e 2 π i=1.
Armed with that knowledge, you need to observe a symmetry. What’s a symmetry? A symmetry is invariance under a transformation: you do something to an
Continue Reading
Up to you. Do you like symmetry? Algebraic symmetry? Geometric symmetry? Polynomials? Fields? There are lots of ways to see this, all valuable.
If you recognize these numbers as the roots of unity of order n n, you can look at answers for this older question.
Let’s suppose you don’t. You don’t know anything about roots of unity or the geometry of complex numbers. But you do know something. You know that a b a c=a b+c a b a c=a b+c, and you know that e 2 π i=1 e 2 π i=1.
Armed with that knowledge, you need to observe a symmetry. What’s a symmetry? A symmetry is invariance under a transformation: you do something to an object, and it stays the same.
For our “object” we’ll take the set of numbers we are adding: those e 2 π i k/n e 2 π i k/n, all of them. Remember: n n is fixed, like 23 23, i i is just the square root of −1−1, but k k varies from 1 1 to n n. There are n n numbers in our set.
Now we transform the set: we multiply each and every one of the numbers by e 2 π i/n e 2 π i/n. It’s one of them, the first one. We sweep it across the set, multiplying it by each member.
What do we get?
That’s right: the same set again. Do you see why? The first number becomes the second, the second becomes the third, and so on, and the last becomes the first, thanks to e 2 π i=1 e 2 π i=1.
We have a symmetry. The set has not changed.
So its sum hasn’t changed.
But its sum also got multiplied by e 2 π i/n e 2 π i/n. That’s the distributive law. You multiply everything by blah, the sum gets multiplied by blah.
So we’re confused.
The sum hasn’t changed, but it also got multiplied by e 2 π i/n e 2 π i/n.
How can that be?
Well it’s fine if e 2 π i/n=1 e 2 π i/n=1, but that only happens when n=1 n=1. What if n>1 n>1?
Well, there is one number – and one number only – which remains unchanged when you multiply it by something that’s not 1 1, and that number is 0 0.
Therefore, the sum must be 0 0. The sum is invariant under multiplication by e 2 π i/n e 2 π i/n, and the only number that’s invariant is 0 0.
If you prefer geometry, you can do the same thing with geometric symmetry.
In the complex plane, these numbers are equally spaced points on the unit circle (the circle of radius 1 1 around the origin). As a set, they are therefore invariant under rotation of the plane by 1/n 1/n of a full turn. Their sum, therefore, is also invariant under such a turn. But there’s only one point in the plane that doesn’t move when you rotate the plane: the origin.
So the sum must be 0 0.
Or maybe you prefer polynomials? The numbers in question are exactly the roots of the polynomial equation X n−1=0 X n−1=0. Therefore their sum is ±± the coefficient of X n−1 X n−1, as it is in any polynomial equation. But X n−1 X n−1 is visibly absent from this polynomial when n>1 n>1. So, the sum is 0 0.
If F F is any field, and M M a nontrivial finite subgroup of the multiplicative group of F F, then the sum of the elements of M M must be 0 0. This can be done in exactly the same way we did the first proof. The present question is the case where the field is C C and M M is the multiplicative group of elements of order n n.
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Jan van Delden
MSc Math and still interested · Author has 4.7K answers and 6.4M answer views
·6y
Originally Answered: How do you prove \displaystyle\sum_{k=1}^ne^{\frac{2\pi ki}{n}}=0 for the positive integer n? ·
It depends.
The summands are the n'th roots of unity.
One general method, for all n n, would be to rewrite this expression, twofold, reindex the roots from 0 0, and express every root as a power of the principal root:
n−1∑k=0 ω k∑k=0 n−1 ω k
with
ω=e 2 π i n ω=e 2 π i n
And for n>1 n>1 we have:
n−1∑k=0 ω k=1−ω n 1−ω=0∑k=0 n−1 ω k=1−ω n 1−ω=0
Since we have ω≠1,ω n=1 ω≠1,ω n=1
If n n is even it might be instructive to draw a unit circle and show that one can split the roots into pairs which add to 0. If root ω k ω k is present, the root ω n−k ω n−k is
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It depends.
The summands are the n'th roots of unity.
One general method, for all n n, would be to rewrite this expression, twofold, reindex the roots from 0 0, and express every root as a power of the principal root:
n−1∑k=0 ω k∑k=0 n−1 ω k
with
ω=e 2 π i n ω=e 2 π i n
And for n>1 n>1 we have:
n−1∑k=0 ω k=1−ω n 1−ω=0∑k=0 n−1 ω k=1−ω n 1−ω=0
Since we have ω≠1,ω n=1 ω≠1,ω n=1
If n n is even it might be instructive to draw a unit circle and show that one can split the roots into pairs which add to 0. If root ω k ω k is present, the root ω n−k ω n−k is also present. The sum of such a pair of roots must be 0 0 since their position is opposite to one another relative to the origin.
If n n is odd, it is not that hard to use a picture to show that the sum of the roots is real. But 0 0 takes more ingenuity.
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11mo
To prove the equality
∑n k=1 e 2 π k i n=0∑k=1 n e 2 π k i n=0
for a positive integer n n, we can use the concept of geometric series and properties of complex exponentials.
Step 1: Recognize the Expression
The expression
e 2 π k i n e 2 π k i n
represents the n n-th roots of unity, excluding k=0 k=0. The sum can be rewritten as:
∑n−1 k=0 e 2 π k i n−e 2 π⋅0 i n=∑n−1 k=0 e 2 π k i n−1∑k=0 n−1 e 2 π k i n−e 2 π⋅0 i n=∑k=0 n−1 e 2 π k i n−1
Step 2: Use the Formula for the Sum of a Geometric Series
The sum of a geometric series is given by:
∑m k=0 r k=1−r m+1 1−r for r≠∑k=0 m r k=1−r m+1 1−r for r≠
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To prove the equality
∑n k=1 e 2 π k i n=0∑k=1 n e 2 π k i n=0
for a positive integer n n, we can use the concept of geometric series and properties of complex exponentials.
Step 1: Recognize the Expression
The expression
e 2 π k i n e 2 π k i n
represents the n n-th roots of unity, excluding k=0 k=0. The sum can be rewritten as:
∑n−1 k=0 e 2 π k i n−e 2 π⋅0 i n=∑n−1 k=0 e 2 π k i n−1∑k=0 n−1 e 2 π k i n−e 2 π⋅0 i n=∑k=0 n−1 e 2 π k i n−1
Step 2: Use the Formula for the Sum of a Geometric Series
The sum of a geometric series is given by:
∑m k=0 r k=1−r m+1 1−r for r≠1.∑k=0 m r k=1−r m+1 1−r for r≠1.
In our case, let r=e 2 π i n r=e 2 π i n and m=n−1 m=n−1:
∑n−1 k=0 e 2 π k i n=1−(e 2 π i n)n 1−e 2 π i n=1−e 2 π i 1−e 2 π i n.∑k=0 n−1 e 2 π k i n=1−(e 2 π i n)n 1−e 2 π i n=1−e 2 π i 1−e 2 π i n.
Step 3: Simplify the Expression
Since e 2 π i=1 e 2 π i=1, we have:
∑n−1 k=0 e 2 π k i n=1−1 1−e 2 π i n=0.∑k=0 n−1 e 2 π k i n=1−1 1−e 2 π i n=0.
Step 4: Conclude the Result
Thus, we find:
∑n−1 k=0 e 2 π k i n=0⟹∑n k=1 e 2 π k i n=0.∑k=0 n−1 e 2 π k i n=0⟹∑k=1 n e 2 π k i n=0.
Therefore, we have proven that
∑n k=1 e 2 π k i n=0.∑k=1 n e 2 π k i n=0.
This holds for any positive integer n n.
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Silvio Capobianco
Mathematician, musician, manatee fan. · Author has 3.3K answers and 611.6K answer views
·Updated 1y
You don’t, because it’s false. For n=1 n=1 the left-hand side is 1 1, not 0 0.
Oh, but maybe you meant: for integer n≥2 n≥2? Well, this you can do with some algebra:
For integer k k between 1 1 and n n both included, the number e 2 π k n=cos 2 π k n+i sin 2 π k i n e 2 π k n=cos2 π k n+i sin2 π k i n is an n n th root of unity, because its n n th power is cos 2 π k+i sin 2 π k=1 cos2 π k+i sin2 π k=1. Then the numbers:
e 2 π i n,e 4 π i n,…,e 2 n π i n e 2 π i n,e 4 π i n,…,e 2 n π i n
(note that the last number is 1 1) are all and only the roots of the polynomial z n−1 z n−1. But in a nonconstant polynomial of degree n n, the trace
Continue Reading
You don’t, because it’s false. For n=1 n=1 the left-hand side is 1 1, not 0 0.
Oh, but maybe you meant: for integer n≥2 n≥2? Well, this you can do with some algebra:
For integer k k between 1 1 and n n both included, the number e 2 π k n=cos 2 π k n+i sin 2 π k i n e 2 π k n=cos2 π k n+i sin2 π k i n is an n n th root of unity, because its n n th power is cos 2 π k+i sin 2 π k=1 cos2 π k+i sin2 π k=1. Then the numbers:
e 2 π i n,e 4 π i n,…,e 2 n π i n e 2 π i n,e 4 π i n,…,e 2 n π i n
(note that the last number is 1 1) are all and only the roots of the polynomial z n−1 z n−1. But in a nonconstant polynomial of degree n n, the trace (that is, the coefficient of degree n−1 n−1 is equal to the sum of the roots of the polynomial, each one taken with its multiplicity, with sign changed.
The trace of z n−1 z n−1 is −1−1 if n=1 n=1, and 0 0 if n≥2 n≥2. So…
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Graham Dolby
Author has 3.2K answers and 1.7M answer views
·May 31
It falls over at the first hurdle: n=1 (a positive integer, as required)
n=1∑k=1 e(2 π k i n)=e 2 π i=1+0 i≠0⊥∑k=1 n=1 e(2 π k i n)=e 2 π i=1+0 i≠0⊥
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It falls over at the first hurdle: n=1 (a positive integer, as required)
n=1∑k=1 e(2 π k i n)=e 2 π i=1+0 i≠0⊥∑k=1 n=1 e(2 π k i n)=e 2 π i=1+0 i≠0⊥
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Daniel Claydon
Learning mathematics · Author has 779 answers and 4.2M answer views
·6y
Originally Answered: How do you prove \displaystyle\sum_{k=1}^ne^{\frac{2\pi ki}{n}}=0 for the positive integer n? ·
Using
e i x=cos(x)+i sin(x)e i x=cos(x)+i sin(x)
we see e 2 i π k≡1 e 2 i π k≡1 for all integers k k. Thus e 2 i π k/n e 2 i π k/n as k k ranges from 1 1 to n n are just the n n th complex roots of unity, satisfying z n−1=0 z n−1=0. From Vieta’s Formulas, the sum of the roots is given by
∑α=−coefficient of z n−1 coefficient of z n=0∑α=−coefficient of z n−1 coefficient of z n=0
and that immediately completes the proof.
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Hélio Waldman
Retired Professor, Collaborating Professor at University of Campinas (UNICAMP) (1973–present) · Author has 481 answers and 462.3K answer views
·6y
Originally Answered: How do you prove \displaystyle\sum_{k=1}^ne^{\frac{2\pi ki}{n}}=0 for the positive integer n? ·
exp[2pii(k+n/2)/n] = exp(2piki/n)exp(pii) = - exp(2piki/n) if i is odd.
So, each element of the summation from k = 1 to n/2 will sum zero with another element from (1+n/2) to n, so the total summation is zero.
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Kurt Behnke
PhD in Mathematics&Theoretical Physics, University of Hamburg (Graduated 1981) · Author has 8.2K answers and 13.9M answer views
·6y
Originally Answered: How do you prove \displaystyle\sum_{k=1}^ne^{\frac{2\pi ki}{n}}=0 for the positive integer n? ·
That is a geometric series, starting at ζ=e 2 π i/n ζ=e 2 π i/n, a primitive nth root of unity. starting with ζ ζ , and with the quotient ζ ζ, too.
The summation formula for geometric series will give you the proof.
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Roman Andronov
A proof lays bare the essence of a problem. · Upvoted by
Allan Steinhardt
, PhD EE, published in various math journals, inventor, hyperbolic Householder · Author has 427 answers and 13.4M answer views
·Updated 7mo
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How do you prove ∫∞0 1 n∑k=0 x k d x=π(n+1)sin(2 π n+1)∫0∞1∑k=0 n x k d x=π(n+1)sin(2 π n+1)?
Reduce And Conquer
Since for the finite sum of the first (n+1)(n+1) consecutive terms of the geometric progression x k x k we have:
n∑k=0 x k=1−x n+1 1−x,x≠1(1)(1)∑k=0 n x k=1−x n+1 1−x,x≠1
the given improper integral I n I n such that:
I n=+∞∫0[n∑k=0 x k]−1 d x(2)(2)I n=∫0+∞[∑k=0 n x k]−1 d x
morphs into the following equivalent:
I n=+∞∫0 1−x 1−x n+1 d x(3)(3)I n=∫0+∞1−x 1−x n+1 d x
Now, purely for the sake of convenience, in the integral I n I n shown in (3) we replace (n+1)(n+1) with n n:
\displaystyle J_n=\int_\limits{0}^{+\infty}\dfrac{1-x}{1-\displaystyle J_n=\int_\limits{0}^{+\infty}\dfrac{1-x}{1-
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Reduce And Conquer
Since for the finite sum of the first (n+1)(n+1) consecutive terms of the geometric progression x k x k we have:
n∑k=0 x k=1−x n+1 1−x,x≠1(1)(1)∑k=0 n x k=1−x n+1 1−x,x≠1
the given improper integral I n I n such that:
I n=+∞∫0[n∑k=0 x k]−1 d x(2)(2)I n=∫0+∞[∑k=0 n x k]−1 d x
morphs into the following equivalent:
I n=+∞∫0 1−x 1−x n+1 d x(3)(3)I n=∫0+∞1−x 1−x n+1 d x
Now, purely for the sake of convenience, in the integral I n I n shown in (3) we replace (n+1)(n+1) with n n:
J n=+∞∫0 1−x 1−x n d x(4)(4)J n=∫0+∞1−x 1−x n d x
and when we are done evaluating J n J n, we simply roll that change back and replace n n with (n+1)(n+1) in the resultant expression for J n J n.
Switching to the complex plane, we consider the following function f(z)f(z):
f(z)=1−z 1−z n(5)(5)f(z)=1−z 1−z n
which is holomorphic everywhere in the complex plane except for the simple poles of f(z)f(z) which are the simple zeros of its denominator 1−z n 1−z n.
That is, the function f(z)f(z) has simple poles, poles of order 1 1, at the n n-th roots of unity ζ k(n)ζ k(n) such that:
ζ k(n)=exp[2 i π k n],k=0,1,2,…,n−1(6)(6)ζ k(n)=exp[2 i π k n],k=0,1,2,…,n−1
Geometrically, to these n n-th roots of unity there correspond the vertices of a regular, origin-centered, n n-gon positioned in the complex plane in such a way that 1) its vertex that corresponds to the root ζ 0(n)ζ 0(n) is located at the point (1,0)(1,0) and 2) the rest of the vertices of the said regular n n-gon are distributed uniformly along the periphery of the origin-centered unit circle with the angular distance of (2 π/n)(2 π/n) radians between the immediately adjacent vertices.
Below, we show the 8 8-th roots of unity, as an example (Fig. 1):
Consequently, in this case we will have at least one real root, ζ 0(n)=1 ζ 0(n)=1 that sits on the (positive branch of the) real axis and if n n is even, as is the case in the diagram above, we will have yet another real root that sits on the (negative branch of the) real axis.
Thus, on the one hand, the stars have prepared for us a couple of indentations on a potential integration contour.
On the other hand, we are the smarter bears and we do not want to futz with more indentations than we have to.
As such, we kraftily kraft a kontour of integration that looks like a slice of pizza with a bite taken out of it with the numbers ε ε and R R chosen so that 0<ε<1 0<ε<1 and R>1 R>1 (Fig. 2):
As the union of 5 5 paths:
γ=5⋃k=1 γ k γ=⋃k=1 5 γ k
we traverse the contour γ γ in the positive, counterclockwise direction.
Here, the central angle delineated by the second n n-th root of unity ζ 1(n)ζ 1(n) is (2 π/n)(2 π/n) radians and we set the central angle delineated by the point A A above to be one half of that angular measure or (π/n)(π/n) radians.
The γ 1 γ 1 and γ 3 γ 3 paths
On the paths γ 1 γ 1 and γ 3 γ 3 we have it that z=x z=x and when R R tends to positive infinity we take the given integral J n J n to be defined in its Cauchy’s principal value sense:
J n=PV∫+∞0 1−x 1−x n d x=lim ϵ→0(∫1−ϵ 0+∫+∞1+ϵ)1−x 1−x n d x(7)(7)J n=PV∫0+∞1−x 1−x n d x=lim ϵ→0(∫0 1−ϵ+∫1+ϵ+∞)1−x 1−x n d x
The γ 2 γ 2 path
On the path γ 2 γ 2 we apply the partial residue theorem: if f(z)f(z) has a simple pole at z 0 z 0 and K K is an arc of a circle |z−z 0|=ϵ|z−z 0|=ϵ with a central angle θ θ then:
lim ϵ→0∮K f(z)d z=θ⋅i⋅Res(f(z),z 0)lim ϵ→0∮K f(z)d z=θ⋅i⋅Res(f(z),z 0)
In our case we are traversing a circular arc γ 2 γ 2 around the point z 0=1 z 0=1, hence the residue of f(z)f(z) at that point is:
Res(f(z),z 0=1)=1−z 0−n z n−1 0=1−1−n=0 Res(f(z),z 0=1)=1−z 0−n z 0 n−1=1−1−n=0
As such, the contribution of the integral over the path γ 2 γ 2 to the grand total vanishes in the ε→0 ε→0 limit:
lim ϵ→0∮γ 2 f(z)d z=0(8)(8)lim ϵ→0∮γ 2 f(z)d z=0
The γ 4 γ 4 path
On the path γ 4 γ 4, where z=R e i θ z=R e i θ with θ θ varying from 0 0 to (π/n)(π/n), in the R→+∞R→+∞ limit our integral vanishes as well.
Indeed, there always exists a positive constant (real number) B B such that whenever |z|=R|z|=R and R R is large then:
|f(z)|⩽B R 2 R n=B R n−2|f(z)|⩽B R 2 R n=B R n−2
Hence, if we demand that n>2 n>2 then:
lim R→+∞B R n−2=0,n>2 lim R→+∞B R n−2=0,n>2
and:
lim R→+∞∮γ 4 f(z)d z=0(9)(9)lim R→+∞∮γ 4 f(z)d z=0
The γ 5 γ 5 path
A lot of fun is happening on the path γ 5 γ 5 where we have it that:
z=r e i π n,d z=e i π n d r z=r e i π n,d z=e i π n d r
with r r varying from R R to 0 0.
Why fun?
Because for the denominator of f(z)f(z) we have:
1−z n=1−r n e i π=1+r n 1−z n=1−r n e i π=1+r n
Isn’t that wonderful?
You bet:
∮γ 5 f(z)d z=−e i π n R∫0 1−r e i π n 1+r n d r(10)(10)∮γ 5 f(z)d z=−e i π n∫0 R 1−r e i π n 1+r n d r
Basically, the path γ 5 γ 5 is the entire magic of this deduction and the rest is just silly arithmetic.
Lastly, glueing all the intermediate pieces together, by the Cauchy’s Residue Theorem, our contour integral must be 0 0 because the contour γ γ contains no poles of f(z)f(z) and that function is holomorphic everywhere on the said contour γ γ:
∮γ f(z)d z=0∮γ f(z)d z=0
and in the ε→0 ε→0 and R→+∞R→+∞ limits we will have:
+∞∫0 1−x 1−x n d x−e i π n+∞∫0 1−r e i π n 1+r n d r=0(11)(11)∫0+∞1−x 1−x n d x−e i π n∫0+∞1−r e i π n 1+r n d r=0
which is to say that:
J n=e i π n+∞∫0 1−r e i π n 1+r n d r=0(12)(12)J n=e i π n∫0+∞1−r e i π n 1+r n d r=0
Some years ago, in this Quora answer, we have proved that:
+∞∫0 x p 1+x n d x=π n⋅1 sin(p+1)π n(13)∫0+∞x p 1+x n d x=π n⋅1 sin[(p+1)π n]
given that:
max(p)=n−2 max(p)=n−2
and we are done since we reduced what we were given, in (4), to a previously solved problem, in (13).
That is:
J n=e i π n I 1−e i π n I 2 J n=e i π n I 1−e i π n I 2
where, by putting p=0 p=0 in (13):
I 1=+∞∫0 1 1+r n d r=π n⋅1 sinπ n(14)I 1=∫0+∞1 1+r n d r=π n⋅1 sin[π n]
and, by putting p=1 p=1 in (13):
I 2=e i π n+∞∫0 r 1+r n d r=e i π n⋅π n⋅1 sin2 π n(15)I 2=e i π n∫0+∞r 1+r n d r=e i π n⋅π n⋅1 sin[2 π n]
Thus, all in all, we have for the integral J n J n:
J n=π n⎡⎢ ⎢ ⎢ ⎢⎣e i π n sin[π n]−e 2 i π n sin[2 π n]⎤⎥ ⎥ ⎥ ⎥⎦J n=π n[e i π n sin[π n]−e 2 i π n sin[2 π n]]
and what remains to be done is some middle school arithmetic.
That is.
From the leftmost sine above we manufacture the sine of a double argument by multiplying both sides of the above leftmost fraction by 2 2 cosines of the given argument (of sine):
J n=π n⎡⎢ ⎢ ⎢ ⎢⎣2 e i π n cos[π n]2 cos[π n]sin[π n]−e 2 i π n sin[2 π n]⎤⎥ ⎥ ⎥ ⎥⎦J n=π n[2 e i π n cos[π n]2 cos[π n]sin[π n]−e 2 i π n sin[2 π n]]
Then, we factor out the reciprocal of the sine of the double argument:
J n=π n 1 sin[2 π n][2 e i π n cos[π n]−e 2 i π n]J n=π n 1 sin[2 π n][2 e i π n cos[π n]−e 2 i π n]
Unwind the above cosine via the exponential functions:
cos[π n]=e i π n+e−i π n 2 cos[π n]=e i π n+e−i π n 2
and cancel everything that can be canceled when multiplying things out:
2 e i π n cos[π n]−e 2 i π n=2 e i π n cos[π n]−e 2 i π n=
e i π n[e i π n+e−i π n]−e 2 i π n=e i π n[e i π n+e−i π n]−e 2 i π n=
=e 2 i π n+1−e 2 i π n=1=e 2 i π n+1−e 2 i π n=1
As such:
J n=π n 1 sin[2 π n]J n=π n 1 sin[2 π n]
Officially:
J n=+∞∫0 1−x 1−x n d x=π n 1 sin2 π n(16)J n=∫0+∞1−x 1−x n d x=π n 1 sin[2 π n]
Lastly, in (16) iterate n n into (n+1)(n+1):
I n=+∞∫0 1−x 1−x n+1 d x=π n+1 1 sin2 π n+1(17)I n=∫0+∞1−x 1−x n+1 d x=π n+1 1 sin[2 π n+1]
or:
I n=+∞∫0[n∑k=0 x k]−1 d x=π n+1 1 sin2 π n+1(18)I n=∫0+∞[∑k=0 n x k]−1 d x=π n+1 1 sin[2 π n+1]
and we are done. □◻
For more information on and ideas about problem-solving in mathematics, physics and computer science please visit my YouTube channel ProbLemma.
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Dean Rubine
Upvoted by
Jeremy Collins
, M.A. Mathematics, Trinity College, Cambridge and
David Joyce
, Ph.D. Mathematics, University of Pennsylvania (1979) · Author has 10.5K answers and 23.2M answer views
·Updated 8y
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How do I prove 1=e 2 π i k 1=e 2 π i k for any integer k k?
Many of the other answers have ‘proven’ this equals −1.−1. Please ignore them.
Euler’s Identity is
e i π=−1 e i π=−1
Squaring, we get what I call Euler’s True Identity:
(e i π)2=(−1)2(e i π)2=(−1)2
e 2 π i=1 e 2 π i=1
Now, for integer k k, we can raise both sides to the k k th power.
(e 2 π i)k=1 k(e 2 π i)k=1 k
e 2 π k i=1 e 2 π k i=1
There it is.
It’s pretty obvious that the statement follows directly from Euler’s Identity. But how do we prove Euler’s Identity? I don’t like the infinite series Euler’s Formula proofs very much. Here’s a calculus proof that avoids Euler’s Formula and goes right to Euler’s Identity.
The plan is to try to integrat
Continue Reading
Many of the other answers have ‘proven’ this equals −1.−1. Please ignore them.
Euler’s Identity is
e i π=−1 e i π=−1
Squaring, we get what I call Euler’s True Identity:
(e i π)2=(−1)2(e i π)2=(−1)2
e 2 π i=1 e 2 π i=1
Now, for integer k k, we can raise both sides to the k k th power.
(e 2 π i)k=1 k(e 2 π i)k=1 k
e 2 π k i=1 e 2 π k i=1
There it is.
It’s pretty obvious that the statement follows directly from Euler’s Identity. But how do we prove Euler’s Identity? I don’t like the infinite series Euler’s Formula proofs very much. Here’s a calculus proof that avoids Euler’s Formula and goes right to Euler’s Identity.
The plan is to try to integrate both sides of an identity, one that ends up with ln ln and the other with arctan arctan and see what happens. We know arctan 1=π/4 arctan1=π/4 which is how we’ll get π π into it.
Let's start with the following expression. It’s a twist on 1+1=2.1+1=2.
1 1+i x+1 1−i x=1+i x+1−i x(1+i x)(1−i x)=2 1+x 2 1 1+i x+1 1−i x=1+i x+1−i x(1+i x)(1−i x)=2 1+x 2
The first step is to integrate. A definite integral gets us the integration constant without a separate step.
∫x 0(1 1+i x+1 1−i x)d x=∫x 0 2 1+x 2 d x∫0 x(1 1+i x+1 1−i x)d x=∫0 x 2 1+x 2 d x
−i ln(1+i x)+i ln(1−i x)|x 0=2 arctan x|x 0−i ln(1+i x)+i ln(1−i x)|0 x=2 arctanx|0 x
With the principal branch of the arctangent, at x=0 x=0 all the terms vanish, so the evaluation endpoints |x 0|0 x just disappear. Let’s combine the logs:
−i ln 1+i x 1−i x=2 arctan x−i ln1+i x 1−i x=2 arctanx
We want to use tan π 4=1.tanπ 4=1. To get an i π i π we need a 4 i 4 i factor on the right, so we multiply both sides by 2 i 2 i.
2 ln 1+i x 1−i x=4 i arctan x 2 ln1+i x 1−i x=4 i arctanx
ln(1+i x 1−i x)2=4 i arctan x ln(1+i x 1−i x)2=4 i arctanx
(1+i x 1−i x)2=e i 4 arctan x(1+i x 1−i x)2=e i 4 arctanx
Now let's let x=1 x=1 so arctan x=π 4.arctanx=π 4.
(1+i 1−i)2=e i π(1+i 1−i)2=e i π
We could divide first. You might notice it’s the ratio of conjugates which always gives double the angle on the unit circle, i i in this case. But it’s easier to square first:
(1+i 1−i)2=1+2 i+i 2 1−2 i+i 2=2 i−2 i=−1(1+i 1−i)2=1+2 i+i 2 1−2 i+i 2=2 i−2 i=−1
Putting it together:
e i π=−1 e i π=−1
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Ján Bábeľa
University degree in Mathematics · Author has 178 answers and 253.5K answer views
·Apr 12
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How do you prove that for even integer n n n∑k=0(−1)k(n k)2 k 2=0∑k=0 n(−1)k(n k)2 k 2=0?
Just some hints:
You may see that (n k)⋅k=n⋅(n−1 k−1)(n k)⋅k=n⋅(n−1 k−1)
So it is equivalent to show that ∑n k=0(−1)k(n k)2=0,∑k=0 n(−1)k(n k)2=0,for odd n n
This is valid, because i-th elements from the begining is the same as i-th element from the end, but with opposite sign.
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Alexey Godin
Ph.D. in Mathematics&Economics, Moscow State University (Graduated 1998) · Upvoted by
Alon Amit
, Lover of math. Also, Ph.D. and
Nathan Hannon
, Ph. D. Mathematics, University of California, Davis (2021) · Author has 2.6K answers and 3.8M answer views
·1y
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How do you prove ∑n k=0(n k)2=(2 n n)∑k=0 n(n k)2=(2 n n), for all n positive integer ?
As it was mentioned in another answer this equality is a generalization of the following lemma:
∑k(n 1 k)(n 2 n 3−k)=(n 1+n 2 n 3)∑k(n 1 k)(n 2 n 3−k)=(n 1+n 2 n 3)
where the summation is for all possible k i.e. k≥0,n 3−k≥0,k≤n 1,n 3−k≤n 2 k≥0,n 3−k≥0,k≤n 1,n 3−k≤n 2
Our statement is just a corollary of this statement with n 1=n 2=n 3=n n 1=n 2=n 3=n because
n∑k=0(n k)2=n∑k=0(n k)(n n−k)=(n+n n)=(2 n n)∑k=0 n(n k)2=∑k=0 n(n k)(n n−k)=(n+n n)=(2 n n)
As for the lemma its proof is a pure combinatorics exercise. Take a pile consisting of n 1+n 2 n 1+n 2 items. We want to know how many ways there are to selec
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As it was mentioned in another answer this equality is a generalization of the following lemma:
∑k(n 1 k)(n 2 n 3−k)=(n 1+n 2 n 3)∑k(n 1 k)(n 2 n 3−k)=(n 1+n 2 n 3)
where the summation is for all possible k i.e. k≥0,n 3−k≥0,k≤n 1,n 3−k≤n 2 k≥0,n 3−k≥0,k≤n 1,n 3−k≤n 2
Our statement is just a corollary of this statement with n 1=n 2=n 3=n n 1=n 2=n 3=n because
n∑k=0(n k)2=n∑k=0(n k)(n n−k)=(n+n n)=(2 n n)∑k=0 n(n k)2=∑k=0 n(n k)(n n−k)=(n+n n)=(2 n n)
As for the lemma its proof is a pure combinatorics exercise. Take a pile consisting of n 1+n 2 n 1+n 2 items. We want to know how many ways there are to select n 3 n 3 of them. This number by the definition is (n 1+n 2 n 3)(n 1+n 2 n 3). On the other hand if we view our big pile as a union of 2 piles one having n 1 n 1 items and the other having n 2 n 2 items we may notice that if we take k k items from the first sub-pile, we need to take n 3−k n 3−k from the second pile to get n 3 n 3 items in total. For any fixed k k the number of ways to take the said number of items is (n 1 k)(n 2 n 3−k)(n 1 k)(n 2 n 3−k). To get the total number of ways I simply need to sum it for all suitable k k.
q.e.d.
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Alon Amit
CS degree and many years of coding. · Upvoted by
Hoosain Ebrahim
, BSc Mathematics & Mathematical Statistics (2021) and
Mathieu Dutour Sikiric
, studied Mathematics & Physics at École Normale Supérieure (1998) · Author has 8.7K answers and 172M answer views
·4y
Related
How can I prove that if n is an integer greater than 1, then ϕ(2 n−1)ϕ(2 n−1) is a multiple of n?
Naming N=2 n−1 N=2 n−1, there’s a multiplicative group (Z/N Z)×(Z/N Z)× of residues mod N N which are relatively prime to N N. The order of this group is φ(N)φ(N).
The residue 2 2 is in this group, since N N is odd. The order of 2 2 in this group is n n, because clearly 2 n≡1(mod N)2 n≡1(mod N) while smaller powers of 2 2 are strictly less than N N. Since the order of an element in a group divides the order of the group, n∣φ(N)n∣φ(N). ■◼
Alternatively, you can use Euler’s theorem to observe that 2 φ(N)≡1(mod N)2 φ(N)≡1(mod N), which means that N N divides 2 φ(N)−1 2 φ(N)−1. In other words
2 n−1∣2 φ(N)−2 n−1∣2 φ(N)−
Continue Reading
Naming N=2 n−1 N=2 n−1, there’s a multiplicative group (Z/N Z)×(Z/N Z)× of residues mod N N which are relatively prime to N N. The order of this group is φ(N)φ(N).
The residue 2 2 is in this group, since N N is odd. The order of 2 2 in this group is n n, because clearly 2 n≡1(mod N)2 n≡1(mod N) while smaller powers of 2 2 are strictly less than N N. Since the order of an element in a group divides the order of the group, n∣φ(N)n∣φ(N). ■◼
Alternatively, you can use Euler’s theorem to observe that 2 φ(N)≡1(mod N)2 φ(N)≡1(mod N), which means that N N divides 2 φ(N)−1 2 φ(N)−1. In other words
2 n−1∣2 φ(N)−1 2 n−1∣2 φ(N)−1
and now use the fact that 2 a−1 2 a−1 divides 2 b−1 2 b−1 precisely when a a divides b b. ■◼
Finally, a more sophisticated proof is possible using the basic theory of finite fields. The multiplicative group of GF(2 n)GF(2 n) is cyclic, and therefore it has φ(2 n−1)φ(2 n−1) generators. The primitive polynomials are the minimal polynomials (over GF(2)(2)) of such generators, and every such primitive polynomial has degree n n and n n roots, each of which is a generator.
Thus the number φ(2 n−1)/n φ(2 n−1)/n is simply the number of primitive polynomials of degree n n, and must be an integer. ■◼
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What is the graph of the function y=2 sin 4x?
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Stuart Herring
Author has 11.7K answers and 8.2M answer views
·4y
Graph the standard sine function first.
Then graph it with a period of π/2 (which is the original period, 2π, divided by the scaling factor 4). (The value at π/4 will be what the original function was at π, for instance.)
Then rescale it vertically by a factor of 2.
Your result should look like this: y=2sin(4x) - Wolfram|Alpha
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Philip Lloyd
Specialist Calculus Teacher, Motivator and Baroque Trumpet Soloist. · Author has 6.8K answers and 52.8M answer views
·1y
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What is the graph of y=1.5 sine 4x?
You first need to know what a basic sine curve is like!
This is y = sin(x) using radians .
If you want degrees put 180 instead of π and 360 instead of 2π
———————————————————————————————————-
——————————————————————————————————————-
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You first need to know what a basic sine curve is like!
This is y = sin(x) using radians .
If you want degrees put 180 instead of π and 360 instead of 2π
———————————————————————————————————-
——————————————————————————————————————-
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The graph of the function y=2 sin(4 x)y=2 sin(4 x) has specific characteristics based on the properties of the sine function. Here's a breakdown of its key features:
Amplitude
The amplitude is the coefficient in front of the sine function, which is 2 2. This means the graph will oscillate between 2 2 and −2−2.
Period
The period of the sine function is determined by the coefficient of x x inside the sine function. The standard period of sin(x)sin(x) is 2 π 2 π. For sin(k x)sin(k x), the period is given by:
Period=2 π k Period=2 π k
In this case, k=4 k=4, so:
Period=2 π 4=π 2 Period=2 π 4=π 2
Phase Shift
There is
Continue Reading
The graph of the function y=2 sin(4 x)y=2 sin(4 x) has specific characteristics based on the properties of the sine function. Here's a breakdown of its key features:
Amplitude
The amplitude is the coefficient in front of the sine function, which is 2 2. This means the graph will oscillate between 2 2 and −2−2.
Period
The period of the sine function is determined by the coefficient of x x inside the sine function. The standard period of sin(x)sin(x) is 2 π 2 π. For sin(k x)sin(k x), the period is given by:
Period=2 π k Period=2 π k
In this case, k=4 k=4, so:
Period=2 π 4=π 2 Period=2 π 4=π 2
Phase Shift
There is no horizontal shift in this function since there is no added constant inside the sine function.
Graph Characteristics
Starts at the origin: The graph starts at (0,0)(0,0).
First peak: The first maximum occurs at x=π 8 x=π 8, where y=2 y=2.
First trough: The first minimum occurs at x=3 π 8 x=3 π 8, where y=−2 y=−2.
Completing the period: The function returns to zero at x=π 2 x=π 2.
Sketching the Graph
To sketch the graph:
Plot the key points: (0,0)(0,0), (π 8,2)(π 8,2), (3 π 8,−2)(3 π 8,−2), and (π 2,0)(π 2,0).
Continue this pattern to the left and right, repeating every π 2 π 2.
Summary
The graph of y=2 sin(4 x)y=2 sin(4 x) will oscillate between 2 2 and −2−2 with a period of π 2 π 2, showing the typical wave-like pattern of the sine function, but with increased frequency and amplitude.
If you need a visual representation, you can use graphing software or online graphing tools to see the exact shape of the graph.
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Robert Colburn
Studied Mathematics at Cabrillo College · Author has 3K answers and 2.4M answer views
·3y
What is the graph of the function y=2 sin 4x?
Looks like a standard sine graph with period = 2pi/4 = pi/2
Amplitude is 2 so the mins and maxs are - 2 and 2
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John Fryer
Author has 890 answers and 885.6K answer views
·4y
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How do I graph the function y=cos x and y=sin (x-π/2)? What’s the relationship between these two graphs?
Graphical Solution
ANSWER
cos x = - sin ( x - π/2 )
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Graphical Solution
ANSWER
cos x = - sin ( x - π/2 )
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Philip Lloyd
Specialist Calculus Teacher, Motivator and Baroque Trumpet Soloist. · Author has 6.8K answers and 52.8M answer views
·6y
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How do you graph sin x = 1/x?
You question should have said, “How can I solve sin(x) = 1/x graphically”.
Then I would have said, draw the graphs of y = sin(x) and y = 1/x the find the intersection points.
Here are the graphs…
The solutions shown are…
Equation Solver:
x=-15.64, y=-0.06392
x=-12.65, y=-0.07908
x=-9.317, y=-0.1073
x=-6.439, y=-0.1553
x=-2.773, y=-0.3607
x=-1.114, y=-0.8975
x=1.114, y=0.8975
x=2.773, y=0.3607
x=6.439, y=0.1553
x=9.317, y=0.1073
x=12.65, y=0.07908
x=15.64, y=0.06392
After this the graph of y = 1/x is so close to the x axis that the solutions are very close to ±6π, ±7π, ±8π, ±9π…
Continue Reading
You question should have said, “How can I solve sin(x) = 1/x graphically”.
Then I would have said, draw the graphs of y = sin(x) and y = 1/x the find the intersection points.
Here are the graphs…
The solutions shown are…
Equation Solver:
x=-15.64, y=-0.06392
x=-12.65, y=-0.07908
x=-9.317, y=-0.1073
x=-6.439, y=-0.1553
x=-2.773, y=-0.3607
x=-1.114, y=-0.8975
x=1.114, y=0.8975
x=2.773, y=0.3607
x=6.439, y=0.1553
x=9.317, y=0.1073
x=12.65, y=0.07908
x=15.64, y=0.06392
After this the graph of y = 1/x is so close to the x axis that the solutions are very close to ±6π, ±7π, ±8π, ±9π…
Upvote ·
99 18
9 2
9 1
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Dave Benson
trying to make maths easy. · Author has 6.1K answers and 2.1M answer views
·Aug 11
Related
How do I graph this function, y=cos (x+90)?
cos(A+B) = cosAcos(90º)-sinAsin(90º) ⟹
cos(x+90º) = -sinx & y = sinx is blue and y = -sinx is red
Continue Reading
cos(A+B) = cosAcos(90º)-sinAsin(90º) ⟹
cos(x+90º) = -sinx & y = sinx is blue and y = -sinx is red
Upvote ·
9 4
Abhijit Tripathy
Former DSA Developer Intern at OpenGenus (2020–2021) · Author has 931 answers and 2.5M answer views
·8y
Related
What is the graph of y=sin^2x?
Let's understand how to draw it without desmos
.
Here first see graph of y=sinX
Now see graph of y=s i n 2 X y=s i n 2 X
What is the difference just portions below x axis in graph y=sinX are just mirrored in above.
So you have to just put the mirror image in case of symmetrical graphs.Hope you understood.
T r i p a t h y.T r i p a t h y.
Continue Reading
Footnotes
Let's understand how to draw it without desmos
.
Here first see graph of y=sinX
Now see graph of y=s i n 2 X y=s i n 2 X
What is the difference just portions below x axis in graph y=sinX are just mirrored in above.
So you have to just put the mirror image in case of symmetrical graphs.Hope you understood.
T r i p a t h y.T r i p a t h y.
Footnotes
Upvote ·
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Jörg Straube
M.Sc. in Computer Science, ETH Zurich (Graduated 1987) · Author has 6.2K answers and 1.7M answer views
·Feb 3
Related
How do you graph the equation y=-4x^2?
When graphing something a first step is a table:
x y = -4x^2
-2 -16
-1 -4
0 0
1 -4
2 -16
By connecting these dots you get the graph:
Continue Reading
When graphing something a first step is a table:
x y = -4x^2
-2 -16
-1 -4
0 0
1 -4
2 -16
By connecting these dots you get the graph:
Upvote ·
9 5
Anurag Singh
B.Tech from Indian Institute of Technology Jammu (Graduated 2020)
·7y
Related
What is the period of the function y=sin^4x + cos^4x?
I have tried to solve you can have a look.
y=(sin²x + cos ²x)²-2sin²xcos²x
=1–1/2(sin2x)²
Period of sin2x is π.
Period of sin²2x is π/2.
So period of y is π/2
And another way is - Period of sin ^4 x is pi and for cos too it is pi but since they are inter convert able functions their period will be pi/2.
Hope it will help.
Upvote ·
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Vishal Chandratreya
graph plotting expert · Author has 931 answers and 2.9M answer views
·5y
Related
What is the graph of y=sin {x} where {.} Denotes functional part?
What is the graph of
y=sin{x}y=sin{x}
where curly brackets denote the functional part function?
The graph of y={x}y={x} is a sequence of slant lines repeating for eternity.
Simply put, it is the portion of y=x y=x in the interval [0,1)[0,1) pasted over and over again.
The sine of these values will give you the graph of y=sin{x}y=sin{x}. In other words, the graph you require is merely the portion of y=sin x y=sinx in the interval [0,1)[0,1) pasted over and over again!
Continue Reading
What is the graph of
y=sin{x}y=sin{x}
where curly brackets denote the functional part function?
The graph of y={x}y={x} is a sequence of slant lines repeating for eternity.
Simply put, it is the portion of y=x y=x in the interval [0,1)[0,1) pasted over and over again.
The sine of these values will give you the graph of y=sin{x}y=sin{x}. In other words, the graph you require is merely the portion of y=sin x y=sinx in the interval [0,1)[0,1) pasted over and over again!
Upvote ·
Vishal Chandratreya
graph plotting expert · Author has 931 answers and 2.9M answer views
·Updated 3y
Related
What is the graph of (sin x)^3?
Is it the behaviour of the function you want? If you only wanted the graph, you could have used a free graphing calculator online.
y=sin 3 x y=sin 3x
It is an odd function, because negating the input negates the output.
sin 3(−x)=[sin(−x)]3=(−sin x)3=−sin 3 x sin 3(−x)=[sin(−x)]3=(−sinx)3=−sin 3x
As a result of this, the maximum and minimum values of this function are the same as those of sin x sinx, and they also occur at the same values of x x.
sin 3 x=⎧⎪ ⎪ ⎪ ⎪⎨⎪ ⎪ ⎪ ⎪⎩−1 x=(4 n−1)π 2 0 x=n π 1 x=(4 n+1)π 2 n∈Z sin 3x={−1 x=(4 n−1)π 2 0 x=n π 1 x=(4 n+1)π 2 n∈Z
The slope of the function is slightly distorted as compared to sin x sinx, being more sluggish to i
Continue Reading
Is it the behaviour of the function you want? If you only wanted the graph, you could have used a free graphing calculator online.
y=sin 3 x y=sin 3x
It is an odd function, because negating the input negates the output.
sin 3(−x)=[sin(−x)]3=(−sin x)3=−sin 3 x sin 3(−x)=[sin(−x)]3=(−sinx)3=−sin 3x
As a result of this, the maximum and minimum values of this function are the same as those of sin x sinx, and they also occur at the same values of x x.
sin 3 x=⎧⎪ ⎪ ⎪ ⎪⎨⎪ ⎪ ⎪ ⎪⎩−1 x=(4 n−1)π 2 0 x=n π 1 x=(4 n+1)π 2 n∈Z sin 3x={−1 x=(4 n−1)π 2 0 x=n π 1 x=(4 n+1)π 2 n∈Z
The slope of the function is slightly distorted as compared to sin x sinx, being more sluggish to increase close to the horizontal axis.
What is the graph of y=(sin x)3 y=(sinx)3?
Upvote ·
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Vital Sine
Math youtuber and student · Author has 102 answers and 111.5K answer views
·4y
Related
How do I graph the function f(x) = sin^2 / x?
As it is typed right now, that is not a valid mathematical expression because the sine function does not have an argument. If you meant sin^2 (x) / x, then you could use a graphing calculator to plot/graph it or desmos, or you could try to do it by hand. You’d need some interval to graph it over though. Intuitively, sine^2(x) oscillates like this:
It is a nonnegative function. Since you are dividing by x, which is negative to the left of y-axis and positive to the right of y-axis, the function sin^2(x)/x will be negative to the left of the y-axis and positive to the right of y-axis, and in fact
Continue Reading
As it is typed right now, that is not a valid mathematical expression because the sine function does not have an argument. If you meant sin^2 (x) / x, then you could use a graphing calculator to plot/graph it or desmos, or you could try to do it by hand. You’d need some interval to graph it over though. Intuitively, sine^2(x) oscillates like this:
It is a nonnegative function. Since you are dividing by x, which is negative to the left of y-axis and positive to the right of y-axis, the function sin^2(x)/x will be negative to the left of the y-axis and positive to the right of y-axis, and in fact, sin^2(x)/x is an odd function, meaning that f(-x) = -f(x) (verify this for yourself). Furthermore, the magnitude of sin^2(x) is bounded, oscillating between 0 and 1, while the magnitude of the denominator, x, will go to infinity, meaning your function’s magnitude will go to zero as x goes to + or - infinity. So intuitively, our graph should look something like this:
That’s a real rough sketch, but here’s what it actually looks like:
So just think about whether your function is odd (symmetric about the origin), or even (symmetric about y-axis), where it is positive and negative, whether it oscillates, etc. If you need to plot over a specific interval, try to find the zeroes of the function, then the zeroes of the derivative (for local maxima/minima), zeroes of the second derivative (for inflection points). Hope that helps.
Upvote ·
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Gorman Aggregation
This document discusses two concepts related to aggregation in economics: 1) Aggregating firms or consumers with identical technologies or preferences can allow representation by a single 'r…
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1 Tw o ele me n tar y re sul ts on agg reg ati on o f tec hno lo-gies and preferences
In what follow s we’ll discuss “agg rega tion”. What do we mean with this term? W e say that an economy admits agg regation if the behavior of the aggregate equilibrium quantities(e.g., aggregate consumption, investment, wealth,...) and prices (e.g., wage, interest rate,...) does not depe nd on the dis tri but ion of the indi vid ual quan tit ies acro ss ag en ts. In other words, we can aggregate whenever we can de
fi
ne a
fi
ctitious “representative agent”that behaves, in equilibrium, as the sum of all individual consumers.
1.1 Ag gr eg at in g
fi
rms with the same technology
Con sid er an eco nom y wit h
fi
rms, ind exe d by
= 1
2
which produce a ho-mogeneous good with the same technology
(
)
where
is aggregate productivity.Assume that
is strictly increasing, strictly concave, di
ff
erentiable in both arguments and const ant retur ns to scale. Can we agg rega te these individu al
fi
rms into a representative
fi
rm?Suppose inputs markets are competitive. Then, each price-taking
fi
rm of type
solves
max
{
}
¡
¢
−
−
(
+
)
with
fi
rst-order conditions
¡
¢
=
+
(1)
¡
¢
=
Recall that by CRS,
and
are homogenous of degree zero, hence:
(
)
(
)=
(
)
(
)
Dividing through the two
fi
rst-order conditions, we obtain
(
)
(
)=
+
and using the fact that the left-hand side is a strictly decreasing function of
(
)
, we obtain
=
µ
+
¶
=
for every
= 1
2
1
iolante/NYUTeach ing/Macrotheory/Spring14/Lectur eNotes/lecture1%2 62_14.pdf
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where capital letters denote averages: every
fi
rm chooses the same capital-labor ratio.Aggregate production across all
fi
rms:
X
=1
¡
¢
=
X
=1
£
¡
¢
+
¡
¢
¤
=
X
=1
[
(
)
+
(
)
]=
(
)
+
(
)
=
(
)
where the last line uses the CRS property of
This derivation proves the existence of a“representative”
fi
rm with technology
(
)
. No te th at
is the same across
fi
rms.With CRS, if one
fi
rm is more productive than all the others, it gets all the inputs.
1.2 Ag gre gat ing co nsu mer s with t he sa me pr efer ence s
Consider a version of the neoclassical growth model with
types of consumers indexed by
= 1
2
with the same endowments of capital
0
=
for all
0
and same preferences
¡
0
1
¢
=
∞
X
=0
(
)
Assume that markets are competitive, so that every consumer faces the same prices. Then,one would think that since all the
consumers make the same decisions, we can aggregate them into a represen tati ve agen t, right? Not so quickl y... Unle ss the utili ty functio n
is strictly concave, agents may not make the same optimal choices of consumption and leisure.Let’s combine these two results on
fi
rms and consumers:
Result 1.0 (trivial aggregation): Suppose that (i) every
fi
rm has the same productivity
and the same CRS production function
, where
is strictly increasing and strictly c onc ave; (ii) co nsum ers have the same initial endowm ents, and same prefe r enc es, and their utility function
is stric tly incr ea sing and stric tly c onc ave. Then, the ne oc lassic al growth model admits a formulation with one representative
fi
rm and one representative household.
2
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2 G or m an ag gr eg at io n
W e no w stu dy a mor e in ter est ing cas e of “de ma nd ag gre ga tti on”, i.e., ag gre gat ion of indivi dual demand curves. Cons ider a stat ic econo my populated by
agents indexed by
= 1
. The comm odity spa ce compris es
consumption goods
©
1
ª
whose price vector is
=
{
}
=1
Each consumer is endowed with
units of wealth, and has utility
, strictly increasing and concave over each of the
goods. All goods ma rk ets are competitive.Consider a particular good
. Aggregate demand of good
is given by the sum of all individual demands, or
(
{
}
) =
X
=1
(
)
which makes it clear that, in general, you need to know the entire distribution of assets across agents to determine aggregate quantities.When can we, instead, write aggregate demand as
(
)
where
=
P
=1
?
In other words, when does aggregate demand only depend on the aggregate endowment,not on its distribu tion. In order for this represen tati on to be true, it must be that if we reallocate one dollar of wealth from consumer
to
, the total demand of
and
does not change, or
(
)
=
(
)
|
=
−
for all
(
)
and for all
This condition is true if all agents have the same marginal propensity to consume out of we alt h, i.e., if the ind ivi dua l dec isi on rul e for consum pti on (re cal l, an out com e of optimization) can be written as
(
) =
(
) +
(
)
(2)Condition
(2)
means that individual Engel curves (individual expenditures as a function of wealth) are linear. Then, aggregate consumption of good
is
(
) = ¯
(
) +
(
)
where
¯
(
) =
P
=1
(
)
3
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This demand aggregation result is due to Gorman (1961), who stated it in terms of indirect utility as follows:
R esult 1.0.1 (Gor man aggr e gation): If (and only if) agent s’ indir e ct utili ty func tions c an b e r epr esen te d as
(
) =
(
) +
(
)
, then aggr eg ate c onsum ption c an be expressed as the choice of a representative agent with indirect utility
(
) = ¯
(
) +
(
)
where
¯
(
) =
P
=1
(
)
That is, for Gorman aggregation what we want is an indirect utility function that can be separated into a term that depends on prices and the consumer’s identity but not on her wealth, and a term that depends on a function of prices that is common to all consu mers that is mu ltipl ied by that consu mer’s wea lth. This indirect utili ty is said to be of the Gorm an for m. Y ou can eas ily pro ve both dir ect ion s (i
ff
) of this result using Ro y’s identit y to obta in the dema nd functi on from the indire ct utility functi on. Recal l that Roy’s identity establishes that
(
) =
−
(
)
(
)
(3)Gorman aggregation (or demand aggregation) is a very powerful result for a number of reasons. First, beyond giving conditions for aggregations, it also explains how to construct the preferences of the representative agent. Moreover, it requires only (somewhat strong)assumptions on the demand side, such as restrictions on
, but no restriction on
fi
nan-cial market s or tec hnolo gy. F or example, we don’t need comp lete
fi
nancia l mark ets. In addition, it is only based on consumer optimization and does not require any equilibrium restrictions.
Quasilinear utility:
W e now consi der an exam ple of Gor man aggreg atio n: agen t
with quasilinear utility over two goods
(
1
2
)
solves
max
{
1
2
}
¡
1
¢
+
2
1
1
+
2
=
where
1
is the relative price —we chose
2
as the numer aire. The FOC s of this probl em 4
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Insertion sort - counting of comparisons and swaps in C
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Asked 9 years, 9 months ago
Modified1 year, 1 month ago
Viewed 27k times
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how can I count number of comparisons and swaps in insertion sort? I have array with 10 random numbers. If somebody help me how to put also 20, 50, 100, 200, 500, 1000, 2000 and 5000 random numbers in this program I will be very happy. I have been thinking of this for a long time and still cannot find solution.
```c
include
include
include
int main()
{
int array;
int i, j, n, temp;
n = 10;
for (i = 0; i < n; i++)
array[i] = rand();
/Sort/
for (i = 1; i < n; i++) {
j = i;
while ((j > 0) && (array[j - 1] > array[j])) {
temp = array[j - 1];
array[j - 1] = array[j];
array[j] = temp;
j--;
}
}
/ Print /
printf("Sorted Array\n");
for (i = 0; i < n; i++)
printf("%d \n", array[i]);
return 0;
}
```
c
count
comparison
swap
insertion-sort
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asked Dec 14, 2015 at 19:07
PetraPetra
23 1 1 gold badge 1 1 silver badge 4 4 bronze badges
2
1 "how can I count number of comparisons and swaps in insertion sort". Increment counters each time you have a comparision or a swap?kaylum –kaylum 2015-12-14 19:45:26 +00:00 Commented Dec 14, 2015 at 19:45
Can you please help me with code?Petra –Petra 2015-12-14 20:12:35 +00:00 Commented Dec 14, 2015 at 20:12
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4 Answers 4
Sorted by: Reset to default
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This is a code by using which you can find out total number of comparisons and swaps in insertion sort
```c
include
#include
#include
int main()
{
int array;
int i, j, n, temp,no_swap=0,comp=0;//variables to find out swaps and comparisons
n = 10;
for (i = 0; i < n; i++)
array[i] = rand(10);
/Sort/
for (i = 1; i < n; i++) {
j = i;
comp++;
while ((j > 0) && (array[j - 1] > array[j])) {
if(array[j-1]>array[j]){
comp++;
}
temp = array[j - 1];
array[j - 1] = array[j];
array[j] = temp;
j--;
no_swap++;//increment swap variable when actually swap is done
}
}
/ Print /
printf("\nNo of swaps = %d",no_swap);
printf("\nNo of comparisions = %d",comp);
printf("\nSorted Array\n");
for (i = 0; i < n; i++)
printf("%d \n", array[i]);
return 0;
}
```
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answered Dec 15, 2015 at 2:55
NutanNutan
786 1 1 gold badge 8 8 silver badges 19 19 bronze badges
2 Comments
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Petra
PetraOver a year ago
Thank you for your help. Does anybody know how to put there also array for 20 then 50, 100, 200, 500, 1000, 2000 and 5000 numbers? I know that I must use dynamic array and I do not know how. I am sorry for my bad english and for my maybe stupid questions but I am beginner.
2015-12-15T14:31:46.713Z+00:00
0
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Nutan
NutanOver a year ago
Just ask user to enter how much array element he/she wants and take that value in n . and declare array with maximum size you want . in your case it is 5000. then use a rand() function to generate values till the n. I hope you know how to take input and use rand() function till the maximum value.....
2015-12-15T16:31:07.34Z+00:00
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This is the code to sort an array using insertion sort and calculate the number of comparisons for best, average and worst case.
```c
include
using namespace std;
int insertionsort( int arr[ ], int n)
{
int i,temp,j;
int comp=0;
for( i=1; i<n ; i++ )
{
temp=arr[i];
j = i - 1;
while( j>=0 && temparr[j])
{
comp++;
}
}
return comp;
}
void display( int arr[ ], int n, int comp )
{
cout<<" Elements of array after sorting "<<endl;
for( int i=0; i<n; i++ )
{
cout<<arr[i]<<" ";
}
cout<<endl;
cout<<" Number of comparisions "<<comp<<endl;
}
int main()
{
int size;
int comp = 0;
cout << " Enter the size of an array " << endl;
cin >> size;
int arr[size];
int n= sizeof(arr) / sizeof(arr);
cout<<" Enter the elements of array "<>arr[i];
}
cout<<" Elements of array before sorting "<<endl;
for( int i=0; i<size; i++ )
{
cout<<arr[i]<<" ";
}
cout<<endl;
int compairsion = insertionsort( arr, n);
display( arr, n, compairson);
return 0;
}
```
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answered Jan 10, 2021 at 16:17
DIGVIJAY SINGH NAYALDIGVIJAY SINGH NAYAL
11 2 2 bronze badges
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Answer by DIGVIJAY SINGH NAYAL is almost correct. To get the correct number of key comparisons, you need to do this:
c
if(j>= 0 && temp>arr[j])
{
comp++;
}
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answered Aug 15, 2024 at 14:50
vyking666vyking666
1 1 1 bronze badge
2 Comments
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Jeremy Caney
Jeremy CaneyOver a year ago
Thank you for being a contributor to the Stack Overflow community. As a question and answer site, Stack Overflow works differently than most message boards. As such, kindly reserve the Answers feature for actual answers, not follow-up comments.
2024-08-23T10:14:03.453Z+00:00
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vyking666
vyking666Over a year ago
Unfortunately, I do not have enough reputation to comment. I simply tried to correct a slight mistake in an otherwise perfect answer.
2024-08-25T09:40:37.383Z+00:00
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Helper functions for the win!
I always prefer to introduce helper functions. Using helper functions allows you to make your code more readable, because everything is split up into smaller pieces.
For example, randomizing the array can be part of a simple function:
c
void randomize( int array, int size )
{
while (size > 0)
array[--size] = rand() % 100;
}
Using it is as simple as:
c
randomize( my_array, my_array_length );
Counting actions
For a simple program like this, it is absolutely OK to add a couple of global variables to track a specific action.
For the actions we wish to track (comparisons and swaps), we only need have a helper function to do each action. That way we do not need to worry about whether or not we got it right in the sort function, because the comparison function itself, for example, only gets invoked when a comparison is being made.
c
int n_comparisons = 0;
int is_greater_than( int a, int b )
{
n_comparisons += 1;
return a > b;
}
Putting it all together
The result is a few more lines of code, but it is significantly more readable.
```c
include
include
include
void randomize( int array, int size )
{
while (size > 0)
array[--size] = rand() % 100;
}
void print( const char title, int array, int size )
{
printf( "%s\n", title );
for (int n = 0; n < size; n++)
printf( " %d", array[n] );
puts("");
}
int n_comparisons = 0;
int is_greater_than( int a, int b )
{
n_comparisons += 1;
return a > b;
}
int n_swaps = 0;
void swap( int a, int b )
{
n_swaps += 1;
int c = a;
a = b;
b = c;
}
void insertion_sort( int array, int size )
{
for (int n_sorted = 1; n_sorted < size; n_sorted += 1)
{
// n is the index of the first UNsorted element,
// which we will shift into its place
int n = n_sorted;
while ((n > 0) && is_greater_than( array[n-1], array[n] ))
{
swap( &(array[n-1]), &(array[n]) );
--n;
}
}
}
int main(void)
{
srand( time(NULL) );
int array;
randomize( array, 10 );
print( "Unsorted:", array, 10 );
insertion_sort( array, 10 );
print( "Sorted:", array, 10 );
printf( "Number of comparisons = %d\n", n_comparisons );
printf( "Number of swaps = %d\n", n_swaps );
return 0;
}
```
Notice another consequence of helper functions: you can do similar things multiple times without having to repeat a whole bunch of code. Here, the print() helper function makes it so much easier to show the array both before and after sorting.
Here is an example run:
Unsorted:
39 27 63 16 29 87 92 70 66 71
Sorted:
16 27 29 39 63 66 70 71 87 92
Number of comparisons = 20
Number of swaps = 13
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answered Aug 15, 2024 at 15:51
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11348 | https://projecteuclid.org/journals/journal-of-applied-mathematics/volume-2012/issue-none/Hamiltonian-Paths-in-Some-Classes-of-Grid-Graphs/10.1155/2012/475087.pdf | Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2012, Article ID 475087, 17 pages doi:10.1155/2012/475087 Research Article Hamiltonian Paths in Some Classes of Grid Graphs Fatemeh Keshavarz-Kohjerdi1 and Alireza Bagheri2 1 Department of Computer Engineering, Islamic Azad University, North Tehran Branch, Tehran, Iran 2 Department of Computer Engineering and IT, Amirkabir University of Technology, Hafez Avenue, Tehran, Iran Correspondence should be addressed to Fatemeh Keshavarz-Kohjerdi, fatemeh.keshavarz@aut.ac.ir Received 8 September 2011; Revised 13 December 2011; Accepted 28 December 2011 Academic Editor: Jin L. Kuang Copyright q 2012 F. Keshavarz-Kohjerdi and A. Bagheri. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
The Hamiltonian path problem for general grid graphs is known to be NP-complete. In this paper, we give necessary and sufficient conditions for the existence of Hamiltonian paths in L-alphabet, C-alphabet, F-alphabet, and E-alphabet grid graphs. We also present linear-time algorithms for finding Hamiltonian paths in these graphs.
1. Introduction Hamiltonian path in a graph is a simple path that visits every vertex exactly once. The prob-lem of deciding whether a given graph has a Hamiltonian path is a well-known NP-complete problem and has many applications 1, 2. However, for some special classes of graphs poly-nomial-time algorithms have been found. For more related results on Hamiltonian paths in general graphs see 3–8.
Rectangular grid graphs first appeared in 9, where Luccio and Mugnia tried to solve the Hamiltonian path problem. Itai et al. 10 gave necessary and sufficient conditions for the existence of Hamiltonian paths in rectangular grid graphs and proved that the problem for general grid graphs is NP-complete. Also, the authors in 11 presented sufficient conditions for a grid graph to be Hamiltonian and proved that all finite grid graphs of positive width have Hamiltonian line graphs. Later, Chen et al. 12 improved the algorithm of 10 and presented a parallel algorithm for the problem in mesh architecture. Also there is a polynomial-time algorithm for finding Hamiltonian cycle in solid grid graphs 13. Recently, Salman 14 introduced alphabet grid graphs and determined classes of alphabet grid graphs which contain Hamiltonian cycles. More recently, Islam et al. 15 showed that the Hamiltoni-an cycle problem in hexagonal grid graphs is NP-complete. Also, Gordon et al. 16 proved that all connected, locally connected triangular grid graphs are Hamiltonian, and gave a 2 Journal of Applied Mathematics sufficient condition for a connected graph to be fully cycle extendable and also showed that the Hamiltonian cycle problem for triangular grid graphs is NP-complete. Nandi et al.
17 gave methods to find the domination numbers of cylindrical grid graphs. Moreover, Keshavarz-Kohjerdi et al. 18, 19 gave sequential and parallel algorithms for the longest path problem in rectangular grid graphs.
In this paper, we obtain necessary and sufficient conditions for the existence of a Ham-iltonian path in L-alphabet, C-alphabet, F-alphabet, and E-alphabet grid graphs. Also, we present linear-time algorithms for finding such a Hamiltonian path in these graphs. Solving the Hamiltonian path problem for alphabet grid graphs may arise results that can help in solving the problem for general solid grid graphs. The alphabet grid graphs that are consid-ered in this paper have similar properties that motivate us to investigate them together. Other classes of alphabet grid graphs have enough differences that will be studied in a separate work.
2. Preliminaries Some previously established results about the Hamiltonian path problem which plays an im-portant role in this paper are summarized in this section.
The two-dimensional integer grid G∞is an infinite graph with vertex set of all points of the Euclidean plane with integer coordinates. In this graph, there is an edge between any two vertices of unit distance. For a vertex v of this graph, let vx and vy denote x and y coordi-nates of its corresponding point. A grid graph G is a finite vertex-induced subgraph of the two-dimensional integer grid. In a grid graph G, each vertex has degree of at most four. A rectangular grid graph Rm, n or R for short is a grid graph whose vertex set is V R {υ | 1 ≤υx ≤m, 1 ≤υy ≤n}. Rm, n is called an n-rectangle. A solid grid graph is a grid graph without holes.
By 10, a vertex v is colored white if υx υy is even, and is colored black otherwise. The size of Rm, n is defined to be mn. Rm, n is called odd sized if mn is odd, and is called even sized otherwise. Two different vertices υ and υ′ in Rm, n are called color compatible if either both υ and υ′ are white and Rm, n is odd sized, or υ and υ′ have different colors and Rm, n is even sized.
An alphabet grid graph is a finite vertex-induced subgraph of the rectangular grid graph of a certain type, as follows. For m, n ≥3, an L-alphabet grid graph Lm, n or L for short, C-alphabet grid graph Cm, n or C for short, F-alphabet grid graph Fm, n or F for short, and E-alphabet grid graph Em, n or E for short are subgraphs of R3m −2, 5n −4.
These alphabet grid graphs are shown in Figure 1, for m 4 and n 3. An alphabet grid graph is called odd sized if its corresponding rectangular graph is odd sized, and is called even sized otherwise.
In the following by Am, n we mean a grid graph Am, n. Let PAm, n, s, t denote the problem of finding a Hamiltonian path between vertices s and t in grid graph Am, n, and let Am, n, s, t denote the grid graph Am, n with two specified distinct vertices s and t of it. Where A is a rectangular grid graph, L-alphabet, C-alphabet, F-alphabet, or E-alphabet grid graph. Am, n, s, t is Hamiltonian if there is a Hamiltonian path between s and t in Am, n. In this paper, without loss of generality we assume sx ≤tx and m ≥n. In the figures, we assume that 1, 1 is the coordinates of the vertex in the lower left corner.
An even-sized rectangular grid graph contains the same number of black and white vertices. Hence, the two end vertices of any Hamiltonian path in the graph must have Journal of Applied Mathematics 3 3m −2 5n −4 a 4n −4 2m −2 m n b m n n 3n −4 2m −2 c n −2 m 2m −4 n n 2n −2 d m n −2 2m −4 n n n 2m −2 e Figure 1: a A rectangular grid graph R10, 11, b an L-alphabet grid graph L4, 3, c an C-alphabet grid graph C4, 3, d an F-alphabet grid graph F4, 3, e an E-alphabet grid graph E4, 3.
s t a s t b s t c s t d Figure 2: Rectangular grid graphs in which there is no Hamiltonian path between s and t.
different colors. Similarly, in an odd sized rectangular grid graph the number of white verti-ces is one more than the number of black vertices. Therefore, the two end vertices of any Ham-iltonian path in such a graph must be white. Hence, the color compatibility of s and t is a nec-essary condition for Rm, n, s, t to be Hamiltonian. Furthermore, Itai et al. 10 showed that if one of the following conditions hold, then Rm, n, s, t is not Hamiltonian: F1 Rm, n is a 1-rectangle and either s or t is not a corner vertex Figure 2a.
F2 Rm, n is a 2-rectangle and s, t is a nonboundary edge, that s, t is an edge and it is not on the outer face Figure 2b.
4 Journal of Applied Mathematics a b Figure 3: A Hamiltonian cycle for the rectangular grid graph R8, 5 and L-alphabet grid graph L4, 3.
F3 Rm, n is isomorphic to a 3-rectangle R′m, n such that s and t are mapped to s′ and t′ and all of the following three conditions hold: 1 m is even, 2 s′ is black, t′ is white, 3 s′ y 2 and s′ x < t′ x Figure 2c or s′ y / 2 and s′ x < t′ x −1 Figure 2d.
A Hamiltonian path problem PRm, n, s, t is called acceptable if s and t are color compatible and R, s, t does not satisfy any of conditions F1, F2, and F3.
The following theorem has been proved in 10.
Theorem 2.1. Let Rm, n be a rectangular grid graph and s and t be two distinct vertices. Then Rm, n, s, t is Hamiltonian if and only if PRm, n, s, t is acceptable.
Lemma 2.2 see 12. Rm, n has a Hamiltonian cycle if and only if it is even-sized and m, n > 1.
Lemma 2.3 see 14. Any L-alphabet grid graph Lm, n m, n ≥3 has a Hamiltonian cycle if and only if mn is even.
Figure 3 shows a Hamiltonian cycle for an even-sized rectangular grid graph and L-alphabet graph Lm, n, found by Lemmas 2.2 and 2.3, respectively. Each Hamiltonian cycle found by these lemmas contains all boundary edges on three sides of the rectangular graph and four sides of the L-alphabet grid graph. This shows that for an even-sized rectangular graph R and L-alphabet graph Lm, n, we can always find a Hamiltonian cycle, such that it contains all boundary edges, except of exactly one side of R and two side of L which contains an even number of vertices.
3. Necessary and Sufficient Conditions In this section, we give necessary and sufficient conditions for the existence of a Hamiltonian path in L-alphabet, C-alphabet, F-alphabet, and E-alphabet grid graphs.
Journal of Applied Mathematics 5 s t L(m, n) R −L e1 e2 a s t b Figure 4: A Hamiltonian path in R10, 11.
Definition 3.1. A separation of i an L-alphabet grid graph Lm, n is a partition of L into two disjoint rectangular grid graphs R1 and R2, that is, V L V R1 ∪V R2, and V R1 ∩V R2 ∅, ii an C-alphabet graph Cm, n is a partition of C into a L-alphabet graph Lm, n and a rectangular grid graph R2m −2, n, that is, V C V L ∪V R2m −2, n, and V L ∩V R2m −2, n ∅, iii an F-alphabet grid graph Fm, n is a partition of F into a L-alphabet grid graph Lm, n and a rectangular grid graph R2m −4, n or four rectangular grid graphs R1 to R4, that is, V F V L ∪V R2m −4, n and V L ∩V R2m −4, n ∅or V F V R1 ∪V R2 ∪V R3 ∪V R4 and V R1 ∩V R2 ∩V R3 ∩V R4 ∅, iv an E-alphabet grid graph Em, n is a partition of E into an F-alphabet grid graph Fm, n and a rectangular grid graph R2m −2, n or a C-alphabet grid graph Cm, n and a rectangular grid graph R2m −4, n, that is, V E V F ∪V R2m − 2, n, and V F ∩V R2m −2, n ∅or V E V C ∪V R2m −4, n, and V C ∩V R2m −4, n ∅.
In the following, two nonincident edges e1 and e2 are parallel, if each end vertex of e1 is adjacent to some end vertex of e2.
Lemma 3.2. Let Am, n be an L-alphabet, C-alphabet, F-alphabet, or E-alphabet grid graph and R be the smallest rectangular grid graph that includes A. If Am, n, s, t is Hamiltonian, then R, s, t is also Hamiltonian.
Proof. We break the proof into two cases.
Case 1 Am, n is an L-alphabet or C-alphabet grid graph. Let P be a Hamiltonian path in L or C that is found by Algorithm 1 or 2. Since R −L or R −C is an even-sized rectangular grid graph of 2m−2×4n−4 or 2m−2×3n−4, then by Lemma 2.2 it has a Hamiltonian cycle i.e., we can find a Hamiltonian cycle of R −L or R −C, such that it contains all edges of R −L or R −C that are parallel to some edge of P. Using two parallel edges of P and the Hamiltonian cycle of R −L or R −C such as two darkened edges of Figure 4a, we can combine them as illustrated in Figure 4b and obtain a Hamiltonian path for R.
6 Journal of Applied Mathematics e1 e2 v1 v2 a s t b s t c Figure 5: A Hamiltonian path in R7, 11.
Case 2. Am, n is an F-alphabet or E-alphabet grid graph. Let P be a Hamiltonian path in F or E that is found by Algorithm 3 or 4. We consider the following cases.
Subcase 2.1 m, n > 3. Since R−F or R−E can be partitioned into three even-sized rectangu-lar grid graphs of R2m−4, n−2, R2, 2n−2, and R2m−2, 2n−2 or R2, 3n−4, R2m−4, n− 2, and R2m −4, n −2, then they have Hamiltonian cycles by Lemma 2.2. Then combine Hamiltonian cycles on R2m−4, n−2, R2, 2n−2 and R2m−2, 2n−2 or R2, 3n−4, R2m− 4, n−2, and R2m−4, n−2 to be a large Hamiltonian cycle and then using two parallel edg-es of P and the Hamiltonian cycle of R−F or R−E, we can obtain a Hamiltonian path for R.
Subcase 2.2 n 3. Let R −F be three rectangular grid graphs of R2m −4, n −2, R2, 2n −2, and R2m −2, 2n −2. We consider the following two subcases.
Subcase 2.2.1 m 3. Let two vertices v1, v2 be in R2m −4, n −2. Using Algorithm 3 there exist two edges e1, e2 such that e1 ∈P or e2 ∈P is on the boundary of Fm, n facing R2m − 4, n−2, see Figure 5a. Hence by combining a Hamiltonian path P and Hamiltonian cycles in R2, 2n−2 and R2m−2, 2n−2 and v1, v2, a Hamiltonian path between s and t is obtained, see Figures 5b and 5c.
Subcase 2.2.2 m > 3. For m 4, let four vertices v1, v2, v3, v4 be in R2m −4, n −2. Using Algorithm 3 there exist four edges e1, e2, e3, e4 such that e1, e2 ∈P, e1, e4 ∈P, e3, e4 ∈P or e2, e3 ∈P are on the boundary of Fm, n facing R2m −4, n −2 see Figure 6a. Therefore, by merging v1, v2 and v3, v4 to these edges and Hamiltonian cycles in R −F we obtain a Hamiltonian path for R, see Figure 6b. For other values of m, the proof is similar to that of m 4.
Similar to F-alphabet grid graphs, Hamiltonian paths can be found in E-alphabet grid graphs for n 3.
Combining Lemma 3.2 and Theorem 2.1 the following corollary is trivial.
Corollary 3.3. Let Am, n be an L-alphabet, C-alphabet, F-alphabet, or E-alphabet grid graph and R be the smallest rectangular grid graph that includes A. If Am, n, s, t is Hamiltonian, then s and t must be color compatible in R.
Journal of Applied Mathematics 7 e1 e2 v1 v2 e3 e4 v3 v4 a s t b Figure 6: A Hamiltonian path in R7, 11.
Therefore, the color compatibility of s and t in R is a necessary condition for Lm, n, s, t, Cm, n, s, t, Fm, n, s, t, and Em, n, s, t to be Hamiltonian.
Definition 3.4. The length of a path in a grid graph means the number of vertices of the path. In any grid graph, the length of any path between two same-colored vertices is odd and the length of any path between two different-colored vertices is even.
Lemma 3.5. Let R2m −2, n and Rm, 5n −4 be a separation of Lm, n such that three vertices v, w, and u are in R2m −2, n which are connected to Rm, 5n −4. Assume that s and t are two given vertices of L and s′ w and t′ t, if s ∈R2m−2, n let s′ s. If tx > m 1 and R2m−2, n, s′, t′ satisfies condition (F3), then Lm, n does not have any Hamiltonian path between s and t.
Proof. Without loss of generality, let s and t be color compatible. Since m, n ≥3 and by Theorem 2.1 a rectangular grid graph does not have a Hamiltonian path only in condition F3, so it suffices to prove the lemma for the case n 3. Assume that R2m −2, n satisfies condition F3. We show that there is no Hamiltonian path in Lm, n between s and t.
Assume to the contrary that Lm, n has a Hamiltonian path P. Since n 3 there are exactly three vertices v, w and u in R2m −2, n which are connected to Rm, 5n −4, as shown in Figure 7a. Then the following cases are possible.
Case 1. t ∈R2m−2, n and s / ∈R2m−2, n. The following subcases are possible for the Hamil-tonian path P.
Subcase 1.1. The Hamiltonian path P of Lm, n that starts from s may enter to R2m−2, n for the first time through one of the vertices v, w, or u, pass through all the vertices of R2m−2, n and end at t, see Figure 7b. This case is not possible because we assumed that R2m −2, n satisfies F3, in this case t′ t and s′ w.
Subcase 1.2. The Hamiltonian path P of Lm, n may enter to R2m −2, n, pass through some vertices of it, then leave it and enter it again and pass through all the remaining vertices of it and finally end at t. In this case, two subpaths of P which are in R2m−2, n are called P1 and P2, P1 from v to u v to w or u to w and P2 from w to t u to t or v to t. This case is not also 8 Journal of Applied Mathematics R(m, 5n −4) v w u R(2m −2, n) a v w u s′ t′ s t b Figure 7: A separation of L4, 3.
possible because the size of P1 is odd even and the size of P2 is even odd, then |P1 P2| is odd while R2m −2, n is even, which is a contradiction.
Case 2 s, t ∈R2m −2, n. The following cases may be considered.
Subcase 2.1. The Hamiltonian path P of Lm, n which starts from s may pass through some vertices of R2m −2, n, leave R2m −2, n at v or u, then passes through all the vertices of Rm, 5n−4 and reenter to R2m−2, n at w go to u or v and pass through all the remaining vertices of R2m−2, n and end at t. In this case by connecting v or u to w we obtain a Hamil-tonian path from s to t in R2m −2, n, which contradicts the assumption that R2m −2, n satisfies F3.
Subcase 2.2. The Hamiltonian path P of Lm, n which starts from s may leave R2m −2, n at v or u, then pass through all the vertices of Rm, 5n −4 and reenter to R2m −2, n at u or v go to w and pass through all the remaining vertices of R2m −2, n and end at t. In this case, two parts of P reside in R2m −2, n. The part P1 starts from s ends at v or u, and the part P2 starts from u or v ends at t. The size of P1 is even and the size of P2 is odd while the size of R2m −2, n is even, which is a contradiction.
Subcase 2.3. Another case that may arise is that the Hamiltonian path P of Lm, n starts from s leaves R2m −2, n at w and reenters R2m −2, n at v or u and then goes to t. But in this case vertex u or v cannot be in P, which is a contradiction. Thus, the proof of Lemma 3.5 is completed.
Lemma 3.6. Let Lm, n and R2m−2, n be a separation of Cm, n such that three vertices v1, w1, and u1 are in R2m−2, n which are connected to Lm, n and x ∈Lm, n is a adjacent vertex to w1.
Assume that s and t are two given vertices of C. If t ∈Lm, n and s ∈R2m −2, n, let s x and s′ w1, t′ s, respectively. If Lm, n, s, t does not have a Hamiltonian path or R2m−2, n, s′, t′ satisfies condition (F3), then Cm, n does not have a Hamiltonian path between s and t.
Proof. The proof is similar to the proof of Lemma 3.5, for more details see Figure 8.
Lemma 3.7. Let Lm, n and R2m−4, n be a separation of Fm, n such that three vertices v1, w1, and u1 are in R2m −4, n which are connected to Lm, n and x ∈Lm, n is an adjacent vertex to Journal of Applied Mathematics 9 L(m, n) v1 w1 u1 s t R(2m −2, n) a L(m, n) x s t w1 R(2m −2, n) s′ t′ s b x L(m, n) s t w1 s′ t′ R(2m −2, n) s c Figure 8: C-alphabet grid graphs in which there is no Hamiltonian path between s and t.
L(m, n) s′ t′ v1 w1 u1 x s t t a L(m, n) w1 x s s t s′ t′ b s t v w u L(m, n) s′ t′ c Figure 9: F-alphabet grid graphs in which there is no Hamiltonian path between s and t.
w1. Assume that s and t are two given vertices of F. If s, t ∈R2m−4, n let s′ s and t′ t; if s (or t) ∈R2m−4, n let s′ w1 and t′ s(or s′ w1 and t′ t); if t(or s) ∈Lm, n let s xt s, s x or t x. If Lm, n, s, t does not have a Hamiltonian path or R2m −4, n, s′, t′ satisfies the condition (F3), then Fm, n does not have a Hamiltonian path between s and t.
Proof. By a similar way as used in the Lemma 3.5 we can prove this lemma; for more details see Figure 9.
Lemma 3.8. Let Fm, n and R2m −2, n or Cm, n and R2m −4, n be a separation of Em, n and s and t be two given vertices in Em, n. If Fm, n, s, t or Cm, n, s, t does not have a Hamiltonian path, then Em, n does not have a Hamiltonian path between s and t.
Proof. The proof is similar to the proof of Lemma 3.5, for more details see Figure 10.
From Corollary 3.3 and Lemmas 3.5, 3.6, 3.7, and 3.8, a Hamiltonian path problem PLm, n, s, t is called acceptable if s and t are color-compatible and R2m −2, n, s′, t′ 10 Journal of Applied Mathematics F(m, n) R(2m −2n, n) s t a C(m, n) s t b Figure 10: E-alphabet grid graphs in which there is no Hamiltonian path between s and t.
does not satisfy the condition F3; PCm, n, s, t is called acceptable if PLm, n, s, t is acceptable and R2m−2, n, s′, t′ does not satisfy the condition F3; PFm, n, s, t is called acceptable if PLm, n, s, t is acceptable and R2m−4, n, s′, t′ does not satisfy the condition F3; PEm, n, s, t is called acceptable if PFm, n, s, t and Cm, n, s, t are acceptable.
Theorem 3.9. Let Am, n be an L-alphabet, C-alphabet, F-alphabet or E-alphabet grid graph. If Am, n, s, t is Hamiltonian, then PAm, n, s, t is acceptable.
Now, we show that all acceptable Hamiltonian path problems have solutions by introducing algorithms to find Hamiltonian paths sufficient conditions. Our algorithms are based on a divide-and-conquer approach. In the dividing phase we use two operations stirp and split which are defined in the following.
Definition 3.10. A subgraph S of an L-alphabet, C-alphabet, F-alphabet or E-alphabet grid graph A strips a Hamiltonian path problem PAm, n, s, t, if all of the following four conditions hold: 1 S is even sized and: i S is a rectangular grid graph; where Am, n is a L-alphabet grid graph Lm, n, a C-alphabet grid graph Cm, n and an E-alphabet grid graph Em, n; ii S is a L-alphabet graph Lm, n, a rectangular graph R2m −4, n or three rectangular grid graphs R1 −R3; where Am, n is a F-alphabet grid graph.
2 S and A −S is a separation of A; 3 s, t ∈A −S; 4 PA −S, s, t is acceptable.
Definition 3.11. Let PAm, n, s, t be a Hamiltonian path problem and p, q be an edge of A, where Am, n is an L-alphabet, C-alphabet, or F-alphabet grid graph. Then we say p, q splits Am, n, s, t if there exists a separation of Journal of Applied Mathematics 11 S L −S s t a S L −S s t b C −S S s t c Figure 11: a, b A strip of L3, 3, c a strip of C3, 3.
Rq p q Rp s t a p q Rp Rq s t b p q Rp Lq s t c Figure 12: a, b A split of L3, 3, c a split of C3, 3.
1 L into Rp and Rq such that i s, p ∈Rp and PRp, s, p is acceptable, ii q, t ∈Rq and PRq, q, t is acceptable.
2 F resp., C into Rp and Lq or Rq and Lpresp., Lq and Rp such that i s, p ∈Rp and PRp, s, p is acceptable or s, p ∈Lp and PLp, s, p is acceptable, ii q, t ∈Lq and PLq, q, t is acceptable or q, t ∈Rq and PRq, q, t is acceptable.
In the following, we describe for each alphabet class how the solutions of the subgraphs are merged to construct a Hamiltonian path for the given input graph.
3.1. Hamiltonian Paths in L-Alphabet Grid Graphs Lm, n Since an L-alphabet graph Lm, n may be partitioned into two rectangular grid graphs, then the possible cases for vertices s and t are as follows.
12 Journal of Applied Mathematics L(m, n) s t R(2m −4, n) a L(m, n) s t R(2m −4, n) b s t R(2m −2, n) F(m, n) c Figure 13: a, b A strip of F4, 3 and F3, 3, c a strip of E3, 3.
L(m, n) s t R(2m −4, n) a s t R1 R2 R3 R4 b s t R1 R2 R3 R4 c Figure 14: A strip of F3, 3, when s, t ∈R2m −4, n.
Case 1 s, t ∈L −S. Assume that L −S has a Hamiltonian path P by the algorithm of 12, where L −S is a rectangular gird graph. Since S is an even-sized rectangular gird graph, then it has Hamiltonian cycle by Lemma 2.2; see Figure 11a. Therefore, a Hamiltonian path for Lm, n, s, t can be obtained by merging P and the Hamiltonian cycle of S as shown in Figure 11b.
Case 2 s ∈Rp and t ∈Rq. In this case, we construct Hamiltonian paths in Rp and Rq between s, p and q, t, respectively; see Figure 12a. Then a Hamiltonian path for Lm, n, s, t can be obtained by connecting two vertices p and q as shown in Figure 12b.
3.2. Hamiltonian Paths in C-Alphabet Grid Graphs Cm, n Similar to L-alphabet graphs since a C-alphabet graph Cm, n may be partitioned into a L-alphabet graph Lm, n and a rectangular grid graph R2m −2, n, then the possible cases for vertices s and t are as follows.
Journal of Applied Mathematics 13 Case 1 s, t ∈C −S. Assume that C −S has a Hamiltonian path P by the Algorithm 1, where C −S is an L-alphabet gird graph Lm, n. Hence, a Hamiltonian path for Cm, n, s, t can be obtained by merging P and the Hamiltonian cycle of S as shown in Figure 11c.
Case 2 s ∈Rp and q ∈Lq. A Hamiltonian path can be found as Figure 12c.
3.3. Hamiltonian Paths in F-Alphabet Grid Graphs Fm, n For F-alphabet grid graphs, we consider the following cases.
Case 1 s, t ∈F −S, where F −S is Lm, n. In this case, we construct a Hamiltonian path between s and t in Lm, n by the Algorithm 1. Since S is an even-sized rectangular grid graph R2m −4, n, then it has a Hamiltonian cycle by Lemma 2.2.
Case 2 s, t ∈F −S, where F −S is R2m −4, n. We construct a Hamiltonian path between s and t in R2m −4, n by the algorithm in 12. Since S is an even-sized L-alphabet grid graph Lm, n, then it has a Hamiltonian cycle by Lemma 2.3.
In two cases, by combining the Hamiltonian cycle of S and the Hamiltonian path of L or R2m −4, n, a Hamiltonian path between s and t for Fm, n is obtained, see Figures 13a and 13b.
Case 3 Fm, n is odd sized and s, t ∈F −S, where F −S is R2m −4, n. In this case, s and t must be white. Since R2m−4, n is even sized, then s and t are not color compatible in R2m− 4, n, see Figure 14a. Therefore, we repartition Fm, n into four rectangular grid graphs R1, R2, R3, and R4, such that s, t ∈V R1 and R2, R3, and R4 are even sized, see Figure 14b where the dotted lines represent the strip. In this case, by combining the Hamiltonian cycles in R2, R3, and R4 and the Hamiltonian path of R1, a Hamiltonian path between s and t for Fm, n, s, t is obtained, see Figure 14c.
Case 4 s ∈Rp and t ∈Lq or s ∈Lp and q ∈Rq. A Hamiltonian path can be found as Figure 15.
3.4. Hamiltonian Paths in E-Alphabet Grid Graphs Em, n A Hamiltonian path for an E-alphabet grid graph Em, n can be found using striping. So we strip Em, n such that s, t ∈E −S, where E −S is F-alphabet Fm, n or C-alphabet Cm, n.
In this case, we construct a Hamiltonian path in Fm, n or Cm, n by Algorithm 3 or 4. Since S is an even-sized rectangular grid graph R2m −2, n or R2m −4, n, then it has a Hamiltonian cycle by Lemma 2.2. By combining the Hamiltonian cycle of S and the Hamiltonian path of F or C, a Hamiltonian path between s and t for Em, n is obtained, see Figure 13c.
Thus, we have the following lemmas.
Lemma 3.12. Let Am, n, s, t be an acceptable Hamiltonian path problem, and S strips it, where Am, n is an L-alphabet, C-alphabet, F-alphabet, or E-alphabet grid graph. If A−S has a Hamiltonian path between s and t, then Am, n, s, t has a Hamiltonian path between s and t.
14 Journal of Applied Mathematics s t L(m, n) R(2m −4, n) a L(m, n) s t p q b s t p q c Figure 15: A split of F3, 3.
procedure L HamiltonianPathLm, n, s, t 1: if L can be stripped then 2: let S be a strip of L, where S is an even-sized rectangular grid graph 3: P ←R HamiltonianPathL −S, s, t 4: D ←HamiltonianCycleS 5: return MergeStripP, D, s, t 6: else 7: let L be split to Rp and Rq 8: P1 ←R HamiltonianPathRp, s, p 9: P2 ←R HamiltonianPathRq, q, t 10: return MergeSplitP1, P2, p, q 11: end if Algorithm 1: The Hamiltonian path algorithm for L-alphabet grid graphs.
Lemma 3.13. Let p, q be an edge which splits PAm, n, s, t. If i Rp, s, p and Rq, q, t, where Am, n is L-alphabet grid graph Lm, n, ii Lq, q, t and Rp, s, p, where Am, n is C-alphabet grid graph Cm, n, iii Rp, s, p and Lq, q, t or Rq, q, t and Lp, s, p, where Am, n is F-alphabet grid graph Fm, n, have a Hamiltonian path between s, p and q, t, then Am, n also has a Hamiltonian path between s and t.
Since all the proofs presented in this section were constructive, they give us algorithms for finding a Hamiltonian path in L-alphabet, C-alphabet, F-alphabet, and E-alphabet grid graphs. The pseudo-codes of the algorithms are given in Algorithms 1, 2, 3, and 4. In these algorithms, HamiltonianCycle is the procedure that finds the Hamiltonian cycle of a strip based on Lemma 2.2 or Lemma 2.3, MergeStrip is a procedure that merges a path and a cycles, MergeCycles is a procedure that combine two Hamiltonian cycles using two parallel edges of e1 and e2, MergeSplit is a procedure that connects two paths by simply adding an edge between their end vertices p and q, and R HamiltonianPath is a procedure that finds Journal of Applied Mathematics 15 procedure C HamiltonianPathCm, n, s, t 1: if C can be stripped then 2: let S be a strip of C, where S is an even-sized rectangular grid graph R2m −2, n 3: P ←L HamiltonianPathC −S, s, t 4: D ←HamiltonianCycleS 5: return MergeStripP, D, s, t 6: else 7: let C be split Rp and Lq 8: P1 ←R HamiltonianPathRp, s, p 9: P2 ←L HamiltonianPathLq, q, t 10: return MergeSplitP1, P2, p, q 11: end if Algorithm 2: The Hamiltonian path algorithm for C-alphabet grid graphs.
procedure F HamiltonianPathFm, n, s, t 1: if F can be stripped, where Fm, n is not odd sized and s, t / ∈R2m −4, n then 2: let S be a strip of F 3: P ←F −S HamiltonianPathF −S, s, t 4: /∗F −S is a L-alphabet grid graph Lm, n or a rectangular grid graph R2m −4, n ∗/ 5: D ←HamiltonianCycleS 6: return MergeStripP, D, s, t 7: else 8: if F can be stripped, where Fm, n is odd sized and s, t ∈R2m −4, n then 9: let S be a strip of F, where S is three rectangular grid graphs R2, R3 and R4 10: P ←R HamiltonianPathR1, s, t 11: c1 ←HamiltonianCycleR3 12: c2 ←HamiltonianCycleR4 13: C ←MergeCyclesc1, c2 14: D ←HamiltonianCycleR2 15: return MergeStripP, D, C, s, t 16: else 17: let F be split to Rp and Lq or Lp and Rq 18: P1 ←R HamiltonianPathRp, s, p 19: P2 ←L HamiltonianPathLq, q, t 20: return MergeSplitP1, P2, p, q 21: end if 22: end if Algorithm 3: The Hamiltonian path algorithm for F-alphabet grid graphs.
a Hamiltonian path in a rectangular grid graph by the algorithm in 12. The algorithm first checks if the input graph A can be stripped, then strips A by S, and recursively finds a Hamiltonian path of A −S. Otherwise, if A can be split, then splits A into Rp and Rq Lq and Rp or Rq and Lp, and recursively finds Hamiltonian paths of Rp and Rq Lq and Rp or Rq and Lp. Then these two Hamiltonian paths are merged into a single path, where Am, n is an L-alphabet, C-alphabet, F-alphabet, or E-alphabet grid graph.
From Theorem 3.9 and Lemmas 3.12 and 3.13 the following theorem holds.
16 Journal of Applied Mathematics procedure E HamiltonianPathEm, n, s, t 1: let S be a strip of E, where S is an even-sized rectangular grid graph R2m −2, n or R2m −4, n 2: P ←E −S HamiltonianPathE −S, s, t 3: /∗E −S is a F-alphabet grid graph Fm, n or a C-alphabet grid graph Cm, n∗/ 4: D ←HamiltonianCycleS 5: return MergeStripP, D, s, t Algorithm 4: The Hamiltonian path algorithm for E-alphabet grid graphs.
Theorem 3.14. Let Am, n be an L-alphabet, C-alphabet, F-alphabet, or E-alphabet grid graph, and s and t be two distinct vertices of it. Am, n has Hamiltonian path if and only if PAm, n, s, t is acceptable.
Theorem 3.14 provides necessary and sufficient conditions for the existence of Hamil-tonian paths in L-alphabet, C-alphabet, F-alphabet and E-alphabet grid graphs.
Combining Theorem 3.14 and the Algorithms 1, 2, 3, and 4 we arrive at the main result.
Theorem 3.15. In L-alphabet, C-alphabet, F-alphabet or E-alphabet grid graphs, a Hamiltonian path between any two vertices s and t can be found in linear time.
Proof. The algorithms divide the problem into some rectangular grid graphs in O1. Then we solve the subproblems in linear time using the linear time algorithm in 12. Then the results are merged in time O1 using the method proposed in 12.
4. Conclusion and Future Work In this paper, we presented linear time algorithms for finding a Hamiltonian path in L-alpha-bet, C-alphabet, F-alphabet, and E-alphabet grid graphs between any two given vertices.
Since the Hamiltonian path problem is NP-complete in general grid graphs, it remains open if the problem is polynomially solvable in solid grid graphs.
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| |~~ |
11350 | https://www.wolframalpha.com/examples/mathematics/mathematical-functions | Wolfram|Alpha Examples: Mathematical Functions
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11351 | https://www.youtube.com/watch?v=cjwBWQRSWQg | Area of Triangles between Parallel Lines
Elroi Academy
12100 subscribers
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Description
1170 views
Posted: 14 Oct 2014
Proving that the area of traingles that share a base between parallel lines are equal
Transcript:
okay now looking at um some triangle area theorems um I'm not going to go into the proof for the area of a triangle we're just going to I suppose assume it um there is a proof so it's not that we're assuming it the same way that we're assuming that the co interior angles are supplementary but we are assuming that the area have a triangle is half the base times the perpendicular height okay basically what we mean by that is that um if I have a triangle I'm just going to draw a few triangles so you can see um I'm going to choose one of the sides as my base so imagine uh this is my base there so if I talk about the half the base it's half of that side um the perpendicular height is how high is the other vertex we call the corners of a triangle vertices okay how high is the other vertex above the the floor that this base is standing on okay so if I draw this a little bit different okay I can maybe have a triangle like this okay there's a triangle so I've chosen this one to be my base this one here is my base and now if I ask what the perpendicular height is I just need to extend my floor a little bit because this is the perpendicular height okay it's how high is this vertex above the floor that this one is standing on does that make sense okay I can't think of another way to draw this uh so I'm going to leave it there but um the next theorem will also illustrate illustrate this quite well okay the theorem says that [Music] triangles um that share a base between parallel lines will have the same [Music] area okay so if I basically what we mean is that if we have two parallel lines well parallel lines of two par we have parallel lines and we draw a triangle between them like that and another triangle that shares a base so that's the first thing they share a base and they are between the parallel lines so this one maybe goes up there to there and these two triangles will have the same area as a matter of fact this might look odd what we mean by having the same area is that if I use paint to color this one I will use the exact same amount of paint to color that okay and if I draw another one here look at this one this is an oddl looking one all the way there okay but it has the same base okay and it's still between these parallel lines you see this triangle very oddl looking one okay skewed one but the amount of painted will use to paint this one or the area of this one will be the same as the area of the others can you guys maybe without even looking into the proof can you tell me why it's it's a very straightforward thing and it follows directly from the definition of of area why would all of them have the same sh well done let's share the same height why do they share the same height exactly that's what we just proved that's why I just proved that it isn't even part of the course really I just first had to show you that that's true so they have the same perpendicular height okay and they share the same base okay so the area to prove this if I have a b c d okay I'm going to start by saying let the per or let H be the peric perpendicular distance [Music] between line a d and BC we know that a d and BC are par parallel and we know from our previous theorem that the distance between this is everywhere the same so I'm just going to say let that distance be a certain value so I'm choosing this funny perpendicular H to be that distance and now to prove it is so simple the area of a b c is equal to a half b c perpendicular height and the area of d b c is also equal to a half b c perpendicular height so we see the same thing happening here we have the same formula for two different areas which means that those two different areas are in fact equal does that make sense okay so pretty soon we're going to step this up quite a few notches okay um it's going to get a little bit difficult very soon |
11352 | https://www.merriam-webster.com/dictionary/intrigue | noun
verb
intrigue
noun
intrigue
verb
transitive verb
intransitive verb
Synonyms
Noun
Verb
plot, intrigue, machination, conspiracy, cabal mean a plan secretly devised to accomplish an evil or treacherous end.
plot implies careful foresight in planning a complex scheme.
an assassination plot
intrigue suggests secret underhanded maneuvering in an atmosphere of duplicity.
backstairs intrigue
machination implies a contriving of annoyances, injuries, or evils by indirect means.
the machinations of a party boss
conspiracy implies a secret agreement among several people usually involving treason or great treachery.
a conspiracy to fix prices
cabal typically applies to political intrigue involving persons of some eminence.
a cabal among powerful senators
plot, intrigue, machination, conspiracy, cabal mean a plan secretly devised to accomplish an evil or treacherous end.
plot implies careful foresight in planning a complex scheme.
intrigue suggests secret underhanded maneuvering in an atmosphere of duplicity.
machination implies a contriving of annoyances, injuries, or evils by indirect means.
conspiracy implies a secret agreement among several people usually involving treason or great treachery.
cabal typically applies to political intrigue involving persons of some eminence.
Examples of intrigue in a Sentence
Word History
Noun and Verb
French intricate affair, from Italian intrigo, from intrigare to entangle, from Latin intricare — see intricate
Noun
1609, in the meaning defined at sense 1b
Verb
1612, in the meaning defined at transitive sense 2
Rhymes for intrigue
Browse Nearby Words
Cite this Entry
“Intrigue.” Merriam-Webster.com Dictionary, Merriam-Webster, Accessed 10 Sep. 2025.
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11353 | https://emergencymedicinecases.com/wp-content/uploads/2019/11/Episode-132-Resloved-Seizure.pdf | 1 Episode 132 Emergency Approach to Resolved Seizures With Drs Paul Koblic & Aylin Reid Prepared by Winny Li & Lorraine Lau, Nov 2019 General approach to the patient with a presumed resolved seizure 1. ABCDEFG (ABC’s and Don’t Ever Forget the Glucose) 2. Establish IV access (for medication delivery if recurrent seizure in the ED) 3. Distinguish between seizure vs seizure mimics 4. Distinguish between first seizure vs recurrent seizure 5. Categorize the seizure 6. Identify the underlying cause of seizure 7. Assess for complications of seizure 8. Assess anti-seizure drug levels 9. Disposition and discharge instructions Step 3: Distinguish between a seizure and seizure mimics Elements that are highly suggestive of true seizure activity include (from highest LR to lowest): 1. Lateral tongue-biting 2. Lateral head rotation 3. Unusual posturing 4. Urinary incontinence 5. Blue skin color observed by bystanders 6. Limb jerking 7. Prodromal trembling, hallucinations, pre-occupation or deja-vu 8. Amnesia for behaviors surrounding event 9. Postictal phase Factors that decrease the likelihood of true seizures 1. Presyncope before LOC 2. LOC with prolonged standing, sitting 3. Prodromal diaphoresis, vertigo, nausea, chest pain, feeling of warmth, palpitations or dyspnea Pearl: Lateral tongue biting has a specificity of 100% for the diagnosis of generalized tonic-clonic seizures in patients who present with a transient loss of consciousness. Distinguishing seizure from syncope All patients who present with a presumed seizure should have an ECG done to assess for causes of cardiac syncope. 2 Distinguishing seizure from psychogenic non-epileptiform seizures (PNES) PNES, formerly “pseudoseizures”, are not due to abnormal electrical activity in the brain. When in doubt, assume true seizure as it can be extremely difficult to distinguish PNES from epileptic seizures in the ED. Video EEG is the gold standard for diagnosis, however this is not typically possible in the ED setting. Epilepsy and PNES frequently coexist in the same patient. It has been estimated that up to 60% of patients with PNES have an addition epileptic seizure disorder. PNES is often misunderstood and patients are perceived as malingering or “faking it”. They have a morbid psychiatric illness. Approach patients with PNES with compassionate counselling and referral for Cognitive Behavioral Therapy, the only therapy proven to be beneficial for PNES. Medications do not effectively prevent or treat the events. Pitfall: Assuming that a seizure is PNES in a patient with a history of PNES. It has been estimated that up to 60% of patients with PNES have an addition epileptic seizure disorder. When in doubt, assume true seizure as can be extremely difficult to distinguish PNES from epileptic seizures in the ED. Distinguishing migraine from seizure While both migraines and seizure tend to have positive neurologic symptoms (increased movement or new sensation) that march, (progress over time and spread through the body) this marching of positive neurologic symptoms occurs over a few seconds in seizures, whereas they occur over several minutes in migraines. 3 Distinguishing TIA from seizure and Todd’s Paralysis While TIAs typically involve a truly abrupt onset of negative neurologic symptoms (loss of sensation or motor function), the symptoms of seizure come on more gradually and generally involve positive neurologic symptoms that march. The exception is Todd’s paralysis. Todd’s paresis/paralysis, defined as transient postictal neurologic deficits, occurs after the seizure, and symptoms can persist from seconds to days before spontaneous resolution. However, both Todd’s paralysis and seizures post-stroke are uncommon presentations. If you aren’t 100% sure why your patient has a persistent new focal neurologic finding after a seizure, or if the story of seizure is unclear, or if the patient is at high risk for a stroke, it is advisable to get on the phone with your stroke team or neurologist to help you sort out whether the patient is a candidate for thrombolysis or endovascular therapy. Can lab values help to distinguish true seizure vs. seizure mimics? Biomarkers such as lactate, CK and ammonia can be helpful as additional data points, but each have their own pros and cons and have ideal time period that they need to be drawn. Lactate Serum lactate appears to peak instantaneously after a seizure and rapidly clears, making it ineffective as a test after 1.5 hours. There may be some discriminating power, but the best cut-off is unclear, and studies are all retrospective with specificities in the 80’s and sensitivities between 65-85%. In certain patient populations with other underlying medical comorbidities such as liver disease or sepsis, they may present with an elevated lactate and have delayed lactate clearance. Nonetheless, a very high lactate within 1.5hrs of seizure that clears completely after 1.5hrs is highly suggestive of a true seizure. CK, ammonia, and prolactin Our experts advise against routinely using other serum biomarkers such as CK, ammonia, and prolactin to rule in or out epileptic seizures. These markers have varying results across studies, with intra and inter-individual variations, and serum levels may be affected by other medical or physiological conditions. Step 4: Distinguish between a first time seizure and recurrent seizure (hint: it’s not just a matter of asking the patient) It is important to distinguish between a first time seizure and recurrent seizure because medical management will change depending on which it is. Ask specifically about subtle motor jerking, positive sensory phenomena, staring spells or hallucinations in the weeks and months prior to presenting to the ED that may suggest an underlying subtle chronic seizure disorder. In one observational study, 28% of patients who presented with a presumed first time generalized tonic-clonic seizure had a history of minor epileptic symptoms such as myoclonus or simple partial seizures. Step 5: Categorize the seizure There are numerous types of seizures that exist that do not need to be identified in the ED as workup and short-term management are not dictated by seizure type. However, it is important to broadly classified seizures in the ED as: 1. Provoked (specific cause) or unprovoked (epilepsy) 2. LOC or no LOC 3. Motor symptoms or not (convulsive or nonconvulsive) 4. Focal or generalized or progress from focal to generalized 4 5. Status epilepticus (> 5min or consecutive seizures without a return to baseline in between) or not Step 6: Identify the underlying cause of the seizure While there are hundreds of causes of seizures, with alcohol withdrawal and epilepsy with drug noncompliance being two of the most common, it is important to rapidly identify the immediate life-threats that require specific time-sensitive antidotes. Immediate life-threats that require immediate treatment with specific antidotes: 1. Vital sign extremes: hypoxemia (O2), hypertensive encephalopathy (labetolol etc) and severe hyperthermia (cooling) 2. Metabolic: hypoglycemia (glucose), hyponatremia (hypertonic saline), hypomagnesemia (Mg), hypocalcemia (Ca) 3. Toxicologic: anticholinergics (HCO3), isoniazid (pyridoxine), lipophilic drug overdose (lipid emulsion) etc. 4. Eclampsia: typically > 20 weeks of pregnancy and up to 8 weeks postpartum (Mg) After any immediate life-threats have been identified and treated it may be useful to divide causes into intracranial vs systemic, and consideration for imaging and lumbar puncture should be entertained. Indications for ED CT head in patients who present with a seizure Consider a non-contrast CT head in patients with a: • First time seizure • Prolonged postictal period or persistent altered mental status • History of malignancy, immunocompromised, bleeding disorder/anticoagulation, shunt, neurocutaneous disorder, chronic alcohol abuse • Fever • Non-trivial head injury • New focal onset seizure • Persistent focal neurological deficit Do all patients with first time seizure require a CT head? Both the American Academy of Neurology and ACEP recommend emergent CT head in adults with first time seizure, noting that CT findings in these patients changes acute management in 9-17% of cases. One study of 259 patients with a first alcohol-related seizure showed a clinically significant CT head lesion in 6.2% of patients even when the history and physical examination were nonfocal. This suggests that patient with a history of alcohol use disorder who present with a seizure should not be presumed to be suffering an alcohol withdrawal seizure as the underlying cause, and that we should have a low threshold for imaging patients with alcohol use disorder with a first-time seizure. Step 7: Assess for complications of the seizure Potential sequelae of seizures include trauma (TBI, long bone fractures, dislocations – posterior shoulder dislocation is a classic injury that often has subtle findings) hypoglycemia, acidosis, rhabdomyolysis, AKI, hyperkalemia, aspiration, neurogenic pulmonary edema, neurogenic cardiac injury (cardiac Takotsubo cardiomyopathy, tachyarrhythmia and sudden unexpected death in epilepsy – SUDEP). Consider serial troponins and ECGs in patients with prolonged seizures or risk factors for CAD as these patients are at risk for developing cardiac ischemia secondary to a seizure. Pearl: An elevated troponin in seizure is NOT a benign post seizure change, it should prompt a cardiac work up! 5 Step 8: Assess anti-seizure drug levels Anti-seizure drug levels are recommended for any patient with known epilepsy/seizure disorder who has a change in their seizure pattern. Factors that affect drug levels and dictate target drug levels include: • Their usual target drug level • Drug compliance • Any new medications that may interact with the anti-seizure medication (eg antibiotics, Wellbutrin) • Change in frequency, duration or features of the seizure • Intercurrent illness that may lower the the seizure threshold Anti-seizure drug levels can be difficult to interpret, especially when multiple drugs are on board, so our experts recommend consulting a neurologist to aid in adjusting drug dosages for all but the noncompliant patient who requires a drug load (see below). Anti-seizure drug concentration assays available to most EDs include: phenytoin, valproate, phenobarbital and carbamazepine. Drug levels that are not immediately available in the ED but may be useful for our neurology colleagues in follow-up include: lamotrigine, levetiracetam (Keppra) and clobazam. Anti-seizure medication drug loading: What’s the evidence? Is Oral or IV better? The ACEP Clinical Policy 2014 suggests that for anti-seizure medications given in the ED setting for patients with a known seizure disorder in which resuming their antiepileptic medication is deemed appropriate, there is a lack of evidence to support one route of administration (oral versus parenteral) over the other in terms of preventing early recurrent seizure. Our experts prefer oral loading because the acute side effects of IV loading may prolong length of stay in the ED. Although loading with antiepileptic medication is commonly done, there is a lack of evidence to support or refute this practice. Should patients with a first time seizure be loaded on an anti-seizure medication in the ED? Our experts agree with the recommendations from the American Academy of Neurology, that first-time unprovoked seizure patients who are back to baseline and suitable for discharge do not require loading on anti-seizure medications. Certain patients at higher risk of recurrent seizures can be considered for medication loading in the ED. For a patient with a first unprovoked seizure clinical factors associated with an increased risk for seizure recurrence include a prior stroke or TBI, a significant neuro-imaging abnormality, or a nocturnal seizure. While the decision to start anti-seizure medications should be individualized, clinicians should advise patients with an unprovoked first seizure that over the longer term (>3 years), immediate treatment is unlikely to improve the prognosis for sustained seizure remission. Our experts recommend Levetiracetam oral load of 1,500mg in the ED followed by 500-1000mg po bid as the drug of choice for ED loading of the first time seizure patient who is deemed appropriate for a drug load because of its effectiveness for both focal and generalized seizures as well as its safety profile. Consider an alternative for patients with known psychiatric illness as levetiracetam may worsen psychiatric symptoms. 6 Step 9: Disposition and discharge instructions of the patient with seizure Which patients with a first-time generalized seizure can be safely discharged home? Those with a single first-time generalized seizure and otherwise normal history and physical who return to neurological baseline can be discharged home with close follow-up with outpatient neurology. If discharged, the patient should have somebody monitor them for recurrent seizure for 24hrs given the significant risk of recurrent seizure (up to 9%). Indications for, and timing of, EEG EEG are useful in confirming epileptic brain activity, defining seizure type and quantifying risk of recurrence. Status epilepticus patients and post status epilepticus patients need an EEG ASAP. Patients with a first unprovoked seizure and patients with a change in their baseline pattern of seizures should get an EEG ideally within a few days, as the diagnostic yield of an EEG decreases with time. Discharge instructions and mandatory reporting for the patient who presents to the ED with a seizure Good discharge instructions can be lifesaving – patients need to know not to swim, bathe alone or a baby in a bathtub, climb heights, operate heaving machinery or drive. In Ontario, it is mandatory to report anyone 16 years of age or older who has had a seizure to the Ministry of Transportation regardless of whether or not they have a driver’s license. Check your local regulations and policies for laws regarding mandatory reporting. 7 Take home points for emergency approach to resolved seizures • ABCDEFG – Don’t Ever Forget the Glucose. • Immediate life threats with specific antidotes: the vital extremes – hypoxemia, hypertensive encephalopathy and hyperthermia, metabolic causes – hypoglycemia, hyponatremia, hypomagnesemia, hypocalcemia, toxicologic causes like TCA, and eclampsia which can occur up to 8 weeks postpartum. • For lab work think about both the causes and the complications of seizures like rhabdomyolysis and acidosis. Consider serial troponins in at-risk patients and serial lactates if you’re not sure if it is a true epileptic seizure. Consider drug levels, both the ones that you can get back immediately and those that might be helpful for the follow up neurologist. • Have a low threshold for CT head for first time seizure patients and for alcoholics who present with withdrawal seizures. • Key elements to distinguish true seizure from seizure mimics include lateral tongue (100% specificity), EMS vital signs of elevated HR and BP, lateral gaze deviation and post-ictal altered mental status. • To distinguish TIA from seizure, TIAs usually have a truly abrupt onset of negative phenomena – a loss of sensation or power vs a seizure or migraine – they march – the motor or sensory symptoms progress over time and migrate through the body, with that marching happening faster in a seizure compared to a migraine. • Todd’s Paralysis is rare, occurs after the seizure and can last seconds to days. If the story is unclear or the patient is at high risk for stroke, it’s advisable to get on the phone with your stroke team or neurologist to help you sort out whether the patient is a candidate for thrombolysis or endovascular therapy. • When in doubt whether or not a seizure was a true epileptic seizure or a psychogenic seizure, err on the side of true seizure – even neurologists with the aid of EEG video monitoring can be fooled. • Drug level interpretation is complicated unless levels are undetectable; consult a neurologist for guidance, especially for patients taking multiple anti-seizure medications • In the ED, oral Keppra is probably the safest choice for loading patients in the ED. • First time unprovoked seizure patients who are back to baseline and suitable for discharge do not require loading on anti-seizure medications. • EEG is indicated for all status epilepticus and post status epilepticus patients ASAP, and within a few days for patients with undiagnosed unprovoked seizures • Good discharge instructions can be lifesaving, and know your local rules around mandatory reporting. References 1. King MA, Newton MR, Jackson GD, Fitt GJ, Mitchell LA, Silvapulle MJ, et al. Epileptology of the first-seizure presentation: a clinical, electroencephalographic, and magnetic resonance imaging study of 300 consecutive patients. Lancet. 1998 Sep;352(9133):1007–11. 2. Sheldon R et Historical criteria that distinguish syncope from seizures. J Am Coll Cardiol. 2002 Jul 3;40(1):142-8. 3. Benbadis SR et al. Value of tongue biting in the diagnosis of seizures. Arch Intern Med. 1995 Nov 27;155(21):2346-9. 4. Krumholz A, Wiebe S, Gronseth G, et al. Practice Parameter: evaluating an apparent unprovoked first seizure in adults (an evidence-based review): report of the Quality Standards Subcommittee of the American Academy of Neurology and the American Epilepsy Society. Neurology. 2007; 69(21):1996-2007. 5. Seizures ACEP Policy committee. Clinical Policy: Critical Issues in the Evaluation and Management of Adult Patients 8 Presenting to the Emergency Department With Seizures. Ann Emerg Med. 2014;63(4):437–447.e15. doi:10.1016/j.annemergmed.2014.01.018. 6. Limdi NA, Shimpi AV, Faught E, et al. Efficacy of rapid IV administration of valproic acid for status epilepticus. Neurology. 2005;64:353-355. 7. Chen L, Feng P, Wang J, et al. Intravenous sodium valproate in mainland China for the treatment of diazepam refractory convulsive status epilepticus. J Clin Neurosci. 2009;16:524-526. 8. Gilad R, Izkovitz N, Dabby R, et al. Treatment of status epilepticus and acute repetitive seizures with i.v. valproate acid vs phenytoin. Acta Neurol Scand. 2008;118:296-300. 9. Marson A, Jacoby A, Johnson A, et al; Medical Research Council MESS Study Group. Immediate versus deferred antiepileptic drug treatment for early epilepsy and single seizures: a randomised controlled trial. Lancet. 2005;365:2007-2013. 10. Chadwick DW. The treatment of the first seizure: the benefits. Epilepsia. 2008;49(suppl 1):26-28. 11. Gottlieb M, Clayton GC. Should Antiepileptic Drugs Be Initiated in the Emergency Department After a First-Time Seizure?. Ann Emerg Med. 2017;69(6):752-754. 12. Leone MA, Giussani G, Nolan SJ, et al. Immediate antiepileptic drug treatment, versus placebo, deferred, or no treatment for first unprovoked seizure. Cochrane Database Syst Rev. 2016;(5):CD007144. 13. An Evidence Based Approach to the First Seizure. Calgary. Supplement – Management of First Time Seizure. Epilepsia, 49(Suppl. 1):50-57, 2008. 14. Doğan EA, Ünal A, Ünal A, Erdoğan Ç. Clinical utility of serum lactate levels for differential diagnosis of generalized tonic-clonic seizures from psychogenic nonepileptic seizures and syncope. Epilepsy Behav. 2017;75:13-17. |
11354 | https://www.jmap.org/JMAPRegentsExamArchives/GEOMETRYCCSSEXAMS/ExamAnswers/0123ExamGEOans.pdf | GEOMETRY The University of the State of New York REGENTS HIGH SCHOOL EXAMINATION GEOMETRY Wednesday, January 25, 2023 -9:15 a.m. to 12:15 p.m., only StudentName: _ .___~y, __ .L-'--6_o/ _ ~ School Name: Ji//J __ A __ _ The possession or use of any communications device is strictly prohibited when taking this examination. If you have or use any communications device, no matter how briefly, your examination will be invalidated and no score will be calculated for you. Print your name and the name of your school on the lines above. A separate answer sheet for Part I has been provided to you. Follow the instructions from the proctor foi completing the student information on your answer sheet. This examination has four parts, with a total of 35 questions. You must answer all questions in this examination. Record your answers to the Part I multiple-choice questions on the separate answer sheet. Write your answers to the questions in Parts II, III, and IV directly in this booklet. All work should be written in pen, except for graphs and drawings, which should be done in pencil. Clearly indicate the necessary steps, including appropriate formula substitutions, diagrams, graphs, charts, etc. Utilize the information provided for each question to determine your answer. Note that diagrams are not necessarily drawn to scale. The formulas that you may need to answer some questions in this examination are found at the end of the examination. This sheet is perforated so you may remove it from this booklet. Scrap paper is not permitted for any part of this examination, but you may use the blank spaces in this booklet as scrap paper. A perforated sheet of scrap graph paper is provided at the end of this booklet for any question for which graphing may be helpful but is not required. You may remove this sheet from this booklet. Any work done on this sheet of scrap graph paper will not be scored. When you have completed the examination, you must sign the statement printed at the end of the answer sheet, indicating that you had no unlawful knowledge of the questions or answers prior to the examination and that you have neither given nor received assistance in answering any of the questions during the examination. Your answer sheet cannot be accepted if you fail to sign this declaration. Notice ... A graphing calculator, a straightedge (ruler), and a compass must be available for you to use while taking this examination. DO NOT OPEN THIS EXAMINATION BOOKLET UNTIL THE SIGNAL IS GIVEN. Al:IJ.311\103E> Part I Answer all 24 questions in this part. Each correct answer will receive 2 credits. No partial credit will be allowed. Utilize the information provided for each question to determine your answer. Note that diagrams are not necessarily drawn to scale. For each statement or question, choose the word or expression that, of those given, best completes the statement or answers the question. Record your answers on your separate answer sheet. [ 48] I In the diagram below, a line reflection followed by a rotation maps b.ABC onto flDEF. --A F~------.0 B c E Which statement is always true? @ BC ::: EF (3) LA ::: LF (2) AC ::: DE (4) LB ::: LD 2 A circle is continuously rotated about its diameter. Which three-dimensional object will be form~ ( 1) cone Ui} sphere (2) prism (4) cylinder Geometry - Jan. '23 Use this space for computations. 3 In the diagram below of 6.CER, LA II CR. E If CL = 3.5, LE = 7.5, and EA = 9.5, what is the length of AR, to the nearest tenth? ~ 5.5 ~4.4 (3) 3.0 (4) 2.8 4 Right trian-gle ABC is shown below. c ~ 8 A Which trigonometric equation is always true for triangle ABC? F) }£ 'S. l2l j_h} . --;y , ; hf 1 )-I~ lf O Geometry - Jan. '23 7 In right triangle LMN shown below, mLM = 90°, MN = 12, and LM = 16. L 16 N M 12 The ratio of cos N is (@12 (3) 12 20 16 (2) 16 (4) 16 20 12 8 In 6.ABC below, DE is drawn such that D and E are on AB and AC, respectively. A If DE II BC, which equation will always be true? (l) AD= DB (3) AD= DE DE BC BC DB f:::\ AD= AB (4) AD= DE ~DE BC BC AB 9 Which polygon does not always have congruent diagonals? (1) square 6)) rhombus · (2) rectangle (4) isosceles trapezoid Geometry - Jan. '23 Use this space for computations. [OVER] Use this space for 10 If the circumference of a standard lacrosse ball is 19.9 cm, what is computations. the volume of this ball, to the nearest cubic centimeter? c 1T " J @ 42 (3) 415 "' CA 133 (4) 1065 c d ~ ;q .. 9 ~~-~~ 1T ) 11 Which polygon always has a minimum rotation of 180° about its center to carry it onto itself? V?J;1T(~;J Rectangle @ /C00° D Square 1Df) (2) Isosceles trapezoid "fJ (3) } 6 D Regular pentagon (4) ~ 1~3 12 Circle 0 is drawn below with secant BCD. The length of tangent AD is 24. o. )-,4 1--1 4 x . q ;x 57 6 5 ~bx'}-16~;. i 9~ x If the ratio of DC:CB is 4:5, what is the length of CB? CF3 ~ S'· lf ,,fD ~ 36 (3) 16 0920 (4) 4 Geometry - Jan. '23 13 The equation of a line is:~-~ 8. ies perpendicular to this line must have a slope of (1) 1. 5 (2) _Q 3 3 (3) --5 @)-~ Use this space for computations. 14 What are the coordinates of the center and length of the radius of the circle whose equation is x2 + y2 + 2x - 16y + 49 = O? ~ ~ I i. C4 l f6 g (1) center( I. -8) and radius 4 x y n--x fl f- I J.- --I 6 yt_ , 1 1 I' @ center (-1,8) and radius 4 / ) l-//:; (3) center (I, -8) and radius 16 I )/ r)) )- J l / - <:/ ~ (4) center (-1,8) and radius 16 [/l :J 15 In the diagram below of right triangle MDL, altitude DG is drawn to hypotenuse ML. D If MG= 3 and GL = 24, what is the length of DG? (1) 8 (2) 9 Geometry - Jan. '23 [OVER] 16 Segment AB is the perpendicular bisector of CD at point M. ~ch statement is always true? (Q)/CB :::: DB (3) i:::,ACD - /:::,BCD (2) CD :::: AB (4) !:::,ACM - i:::,BCM 17 In the diagram below of circle 0, AC and BC are chords, and mLACB = 70°. B If OA = 9, the area of the shaded sector AOB is (1) 3.51t (2) 71t Geometry - Jan. '23 (3) 15.751t ®31.51t A Use this space for computations .. c Use this space for 18 Quadrilateral BEST has diagonals that intersect at point D. Which computations. statement would not be sufficient to prove quadrilateral BEST is a parallelogram? } (1) BD ::: SD and ED ::: TD lJ f A./{} n a.,/ 5 b i '})-b 19 The equation of line tis 3x - y = 6. Line mis the image of line t after a dilation with a scale factor of ~ centered at the origin. What is an equation of line m? (1) y = ~ x - 3 (2) y = ~ x - 6 (3) y = 3x + 3 @y=3x-3 r/~ g 20 A cylindrical pool has a diameter of 16 feet and height of 4 feet. The pool is filled to ~ foot below the top. How much water does the pool contain, to the nearest ga~lo ? [l ft3 = 7.48 gallons] (1) 704 (3) 5264 (2) 804 4) 6016 Geometry - Jan. '23 v~rrr').-h ~ 1T{~f()-1-o.r;) ., ))--Y 1f /.J .. lf 1f . 7- 4 y ~ ) J-bll [OVER] 21 The area of /:::,.TAP is 36 cm2. A second triangle, JOE, is formed by connecting the midpoints of each side of /:::,.TAP. What is thyrea of ){OE, in square centimeters? : I \uj)g (3) 18 J 0 (2) 12 (4) 27 A 22 On the set of axes below, the endpoints of AB have coordinates A(-3,4) and B(5,2). y x If AB is dilated by a scale factor of 2 centered at (3,5), what are the coordinates of the endpoints of its image, A' B'? Use this space for computations. (1) A'(-7,5) and B'(9,l) ~ A'(-6,8) and B'(l0,4) (2) A' ( - 1,6) and B '(7,4) ~A' ( -9,3) and B' (7, - 1) (~ q ) Al-\Y) ~ l-'1~ !) --'/ (/;,~;} __.?) . I 3 8lS)1-)-5/(l/;)--'? {}t;/b)--? {7) ~1) Geometry - Jan. '23 23 In the circle below, AD, AC, BC, and DC are chords, EDF is Use this space for computations. tangent at point D, and AD II BC. 5,n~AO JJ~ M~ G i-Al8 ,-; f fVl /f8 LCDf~ i_m Gp Which statement is always true? jR LADE :::::: LCAD U:YLCDF:::::: LACB (3) LBCA :::::: LDCA (4) LADC:::::: LADE 24 In the diagram below of .6.ABC, D and E are the midpoints of AB and AC, respectively, and DE is drawn. A I. AA similarity rey ~ 60-.t(,, J ;I_ Of{6 fl' fVoof~) II. SSS similaritf111e,,'~~,ay~>J~Y1Vf 111 sJ~$ ( J III. SAS similarity ').. wrrt >; () Mi Vij' g IM. j ~ jJ ~~fr-v fl;?) Which methods could be used to prove fl.ABC- fl.ADE? f' / ti. l";j /£ /J -~V~} (1) I and II, only f.t\I and III, only (2) II and III, only ~I, II, and III Geometry - Jan. '23 [OVER] Part II Answer all 7 questions in this part. Each correct answer will receive 2 credits. Clearly indicate the necessary steps, including appropriate formula substitutions, diagrams, graphs, charts, etc. Utilize the information provided for each question to determine your answer. Note that diagrams are not necessarily drawn to scale. For all questions in this part, a correct numerical answer with no work shown will receive only I credit. All answers should be written in pen, except for graphs and drawings, which should be done in pencil. 25 Using a compass and straightedge, construct the angle bisector of LABC. [Leave all construction marks.] B c Geometry - Jan. '23 26 On the set of axes below, MBC and !::.DEF are graphed. y x Describe a sequence of rigid motions that would map MBC onto !::.DEF. ~ t fip !Lot ,qe, qo 0 v/or.Jrvi·ye ab~vt- P 'l ,Y) . . ) J LL ~ y I fl h+ /, ff A, h) tJ-fe vtDVVY' T J Geometry - Jan. '23 . [OVER] 27 As shown in the diagram below, a symmetrical roof frame rises 4 feet above a house and has a width of 24 feet. 4ftI~ l )--- 24 ft Determine and state, to the nearest degree, the angle of elevation of the roof frame. ta vi G ~ -% t) ~ J? Geometry-Jan. '23 28 Directed line segment AB has endpoints whose coordinates are A(-2,5) and B(8, -1). Determine and state the coordinates of P, the point which divides the segment in the ratio 3:2. [The use of the set of axes below is optional.] -J-r}(YrJ-) ~ -J--rfU0):: -J-+b"Y s ,rl-C-1-s) ~ c; ti-(b)-: s -l} 5 ., ?5- -JJ_ !L ;J s s Ci, --s) ,, f y x Geometry-Jan. '23 [OVER] 29 In !:,ABC, AB= 5, AC= 12, and mLA = go 0 • In !:,DEF, mLD = go 0 , DF = 12, and EF = 13. Brett claims !:,ABC ~ !:,DEF and !:,ABC ~ !:,DEF. 555 Geometry - Jan. '23 30 The volume of a triangular prism is 70 in3. The base of the prism is a right triangle with one leg whose measure is 5 inches. If the height of the prism is 4 inches, determine and state the length, in inches, of the other leg of the triangle. Geometry - Jan. '23 70 ~ ~(J){L){~ 70,, lOL 7~~ [OVER] 31 Triangle ABC with coordinates A(-2,5), B(4,2), and C(-8, -1) is graphed on the set of axes below. y Determine and state the area of MBC. At-<'-t"- 0 ( O c OE'. ( : 61 ))--< 71-A )-U' o( h CD I? '. lJ--p- {1 g Ar0 o( .L1 f'A G ; ~ ~)3 ;1yuor£iAEl5' ~,,(°f) J-7 Geometry - Jan. '23 Part III Answer all 3 questions in this part. Each correct answer will receive 4 credits. Clearly indicate the necessary steps, including appropriate formula substitutions, diagrams, graphs, charts, etc. Utilize the information provided for each question to determine your answer. Note that diagrams are not necessarily drawn to scale. For all questions in this part, a correct numerical answer with no work shown will receive only I credit. All answers should be written in pen, except for graphs and drawings, which should be done in pencil. 32 Sally and Mary both get ice cream from an ice cream truck. Sally's ice cream is served as a cylinder with a diameter of 4 cm and a total height of 8 cm. Mary's ice cream is served as a cone with a diameter of 7 cm and a total height of 12.5 cm. Assume that ice cream fills Sally's cylinder and Mary's cone. Bern Sally's 4cm 12.5 cm Mary's 7cm Whowas•e;(~i~{ij:IOO!}Jusr~{]: [) J LA N & j s Lt o !). /J)1 / > 0 > CJV M~ tNv OYl~(ven+ a.11~ h>. Determine and state, to the nearest foot, the height of the tree. cos OD ~ (s 1a. vi lJ{) ,, ~ x ~)Lt,?! y' ~ ?tf Geometry - Jan. '23 [OVER] Part IV Answer the question in this part. A correct answer will receive 6 credits. Clearly indicate the necessary steps, including appropriate formula substitutions, diagrams, graphs, charts, etc. Utilize the information provided to determine your answer. Note that diagrams are not necessarily drawn to scale. A correct numerical answer with no work shown will receive only 1 credit. All answers should be written in pen, except for graphs and drawings, which should be done in pencil. [ 6] 35 Given: Triangle DUG with coordinates D( -3, -1), U( -1,8), and C(8,6) Prove: 6.DUC is a right triangle [The use of the set of axes on the next page is optional.] cg-- f i) -: rf 1 DJ (; ~ l - (-2;) Geometry - Jan. '23 Question 35 is continued on the next page. Question 35 continued Point U is reflected over DC to locate its image point, U', forming quadrilateral DUCU'. Prove quadrilateral DUCU' is a square. ) lYlc.R., 0 /) fo/Jv }1 ks \j/ LDUC ;s CA r;qh-+ a 51 var< y Geometry - Jan. '23 x |
11355 | http://garytuttle.ee/circuits/topics/ac_the_impedance_way.pdf | EE 201 AC — the impedance way – 1 AC circuit analysis The story so far: 1. For circuits that are driven by sinusoidal sources (e.g. vs(t) = Vm·cos(ωt) ), the voltages and currents are always sinusoids oscillating at the same frequency as the source and having distinct amplitudes. If there are capacitors and inductors in the circuit then the sinusoidal voltages and currents may also have phase shifts with respect to the source. These sinusoids, with the various amplitude and angles, are easy to see and measure in the lab.
2. Calculating the amplitudes and phase angles using conventional differential-equation techniques is messy and may involve a lot of trigonometric gymnastics.
3. If we ignore transients effects and focus on the steady-state part of the solution, the math is made easier by leaving out half of the problem. This is known as sinusoidal steady-state analysis.
4. If we describe the sinusoids using complex exponentials (Vm·ejωt) instead of sines and cosines, the math needed to solve the differential equations is easier. But there is a tradeoff — we have introduced complex numbers. Complex math is messy, but the complex form provide a compact way to describe the amplitude and phase shift information of the sinusoidal voltages and currents. They are convenient, if we learn how to use them.
EE 201 AC — the impedance way – 2 iR (t) = Vmejωt R = vR (t) R vR (t) iR (t) = R iC (t) = C d (Vmejωt) dt = jωC [vC (t)] vC (t) iC (t) = 1 jωC iL (t) = 1 L ∫Vmejωtdt = vL (t) jωL vL (t) iL (t) = jωL But there is more to this business of using complex numbers. To see it, apply a complex exponential voltages to individual resistors, capacitors, and inductors and find expressions for the resulting currents.
👀 !!
Big deal. It’s just Ohm’s law.
Wut !?!
Vmexp(jωt) + – i(t) R Vmexp(jωt) + – i(t) C Vmexp(jωt) + – i(t) L EE 201 AC — the impedance way – 3 In each case, the sinusoidal voltage results in a sinusoidal current — no big surprise here. What is surprising is that, for each component, the ratio of the of sinusoidal voltage to the sinusoidal current is a number. Of course, we expect this for resistors because they obey Ohm’s law, but capacitors and inductors do not follow Ohm’s law. Yet, with sinusoids, there is a quantity that behaves almost like resistance. We call the quantity the impedance. Using impedance allows us to treat resistors, capacitors, and inductor in sinusoidal circuits in a unified manner.
i (t) = vS (t) Z + – Z i(t) vS (t) = Vm ⋅ejωt resistor: capacitor: inductor: Z = R Z = 1 jωC Z = jωL EE 201 AC — the impedance way – 4 Impedance Impedance is complex, so it carries magnitude and phase angle information.
resistor: capacitor: inductor: iR = vR Z = vR R = ( vR R ) ej0∘ iC = vC ZC = vC 1 jωC = (jωC) vR = (ωC ⋅vC) ej90∘ iL = vL ZL = vL jωL = ( vL ωL ) e−j90∘ For the resistor, the current is exactly in phase with voltage. For the capacitor, the current leads the voltage by 90°. For the inductor, the current lags the voltage by 90°.
These observations are in line with what we saw when using sines and cosines to describe oscillations. The derivatives in the capacitor and inductor i-v relations turned sines to cosines and vice-versa.
Since impedance is defined as voltage divided by current, the units must be ohms.
EE 201 AC — the impedance way – 5 Impedance The capacitor and inductor impedances are purely imaginary, and are referred to generally as reactances. We note that inductor and capacitor impedances have opposite signs. So for circuits that have inductors and capacitors, the impedances may tend to cancel each other. It is possible that they may cancel exactly (ZL = –ZC) — a situation that we call resonance. This “fight” between inductor impedance and capacitive impedance has important implications and applications. We will study some of these later in 201 and in EE 230.
Equally important is the frequency dependence of the two impedances. The inductor impedance increases proportionally with increasing frequency, the capacitor impedance decreases inversely with increasing frequency — exact opposites.
ZL = jωL ZC = 1 jωC = −j ( 1 ωC) One-line proof: 1 j = 1 ej90∘= e−j90∘= −j EE 201 AC — the impedance way – |Z| ω 6 ZR ZC ZL Frequency dependence of the magnitudes of the three impedances.
Resistors are frequency independent. Capacitors and inductors change behavior as the frequency changes. Having all three impedances meet at a single frequency, as shown in this graph would be unusual. But we could certainly force that to happen by making appropriate choices for R, L, C, and ω!
EE 201 AC — the impedance way – 7 ZL = jωL ZC = 1 jωC At very low frequencies (ω → 0, which is just another way of describing DC), |ZL| → 0 and |ZC| → ∞. At DC, the inductor becomes a short circuit and the capacitor becomes an open circuit. This is not a surprise — this is exactly how we introduced the inductor and capacitor. At DC, an inductor is a fancy short circuit and a capacitor is fancy open circuit.
But at very high frequencies (ω → ∞), the situation is quite different: |ZL| → ∞ and |ZC| → 0!
The inductor and capacitor have completely switched roles. This is quite unexpected. Obviously, the ways that impedance changes with frequency will have a big impact on how a circuit behaves at different frequencies.
EE 201 AC — the impedance way – 8 + – C – + R1 R2 L Consider this RLC circuit. VS is a sinusoid.
VS v2 Suppose the frequency is very low, ω → 0. (i.e. DC.) The inductor behaves like a short and the capacitor like an open.
VS v2 = R2 R1 + R2 VS Now let the frequency be very high, ω → ∞. The inductor behaves like a open and the capacitor like a short!
+ – R1 R2 – + v2 = 0!
VS + – R1 R2 – + Using the frequency dependence of the impedances is an important part of manipulating and processing signals. (EE 230, EE 224) EE 201 AC — the impedance way – 9 Impedances give us the opportunity to re-use the circuit analysis techniques that we learned at the beginning of 201. Recall that we combined Kirchoff’s Laws together with Ohm’s Law to solve many different resistive DC circuits using a variety of methods. Impedances are quantities that relate voltages and currents in exactly same way as resistors. This implies that we could use impedances together with Kirchoff’s Laws to solve AC circuits, using the same methods (dividers, node voltage, mesh current, etc.) that we learned earlier. Except that now the calculations will be done using complex numbers. We take on the burden of complex math so that we can return to our familiar circuit analysis methods and stop solving messy differential equations.
So our AC analysis approach will be to first convert the AC circuit to its complex equivalent. (Sources become complex sinusoids and components become impedances.) Then we ask ourselves the question: “If the impedances were all resistors, what method would we use to find DC voltages and currents?” Then we apply that method using impedances instead of resistors. There will be complex math involved — maybe a little or maybe a lot. When we get through that, the results will be complex voltages and currents, which tell us the amplitudes and phase angles of the sinusoids.
Using impedances to analyze AC circuits EE 201 AC — the impedance way – 10 The procedure for solving AC circuits using impedances is: 1. Convert the sources to exponential sinusoids. If there is only one source, we can choose its phase to be zero. If there are multiple sources, we will need to keep track of any phase differences between them.
2. Convert the components to impedances.
3. Use the usual collection of tools (dividers, node voltage, mesh current, etc.) to set up equations relating voltages and currents in the circuit.
4. Grind through the complex algebra to find the complex values for the voltages and currents. (This is the worst part.) 5. When finished, express the complex voltages and currents in magnitude and phase form. The magnitude is amplitude of the oscillation and the phase is the shift relative to the source. These are the features that we would observe if the we built the circuit in the lab and used an oscilloscope to view the sinusoidal wave forms.
Following are many examples, starting with a slew of dividers.
EE 201 AC — the impedance way – 11 Example 1 Transform to the complex version of the circuit.
ZR = R ZC = 1 jωC vC = ZC ZR + ZC [Vm exp (jωt)] Use AC analysis to find the sinusoidal form of the resistor voltage below.
In viewing the complex circuit and thinking about how to approach it if the impedances were all resistors, it seems that using a voltage divider would be a reasonable approach.
+ – R C – + vC (t) vS (t) = Vm cos (ωt) 1 kΩ 0.1 µF Vm = 5 V ω = 10,000 rad/s + – – + vC ZR ZC Vm exp (jωt) EE 201 AC — the impedance way – 12 Working out the value for the voltage divider ratio: Mind the negatives. (1/j = –j !) Plug in the numbers. Convert to magnitude/phase. Finish.
Then the resistor voltage is ZC ZR + ZC = 1 jωC R + 1 jωC = −j ( 1 ωC) R −j ( 1 ωC) = −j1000 Ω 1000 Ω −j1000 Ω = (1000 Ω) e−j90∘ (1414 Ω) e−j45∘ = (0.707) e−j45∘ vR = [(0.8) e−j36.9∘ ] [(5 V) exp (jωt)] = (4 V) ej(ωt −36.9∘) EE 201 AC — the impedance way – 13 Plugging in numbers early in the calculation is OK, but sometimes the complex math is a little easier if we do a bit more algebra with symbols before switching to numbers. We might also gain some insight what is going on in the circuit. Go back to the voltage divider ratio: Multiply top and bottom by jωC. Now plug in the numbers And we get the same ratio.
In this case, there is not a huge difference in the math process, but we do see a simplification that comes from using dimensionless quantities. (Note that ωRC is dimensionless — check the units.) vR = (4 V) ej(ωt −36.9∘) ZC ZR + ZC = 1 jωC R + 1 jωC = 1 1 + jωRC = 1 1 + j1 = 1 1.414 ⋅ej45∘= 0.707 ⋅e−j45∘ The result is a sinusoid with amplitude of 4 V, shifted in phase by –36.9° from the source. EE 201 AC — the impedance way – 14 Example 2 + – L R – + vR (t) vS (t) = Vm cos (ωt) Transform to the complex version of the circuit.
+ – – + vR ZL ZR Vm exp (jωt) ZR = R ZL = jωL vL = ZR ZR + ZL [Vm exp (jωt)] Use AC analysis to find the sinusoidal form of the resistor voltage below.
Again, using a voltage divider seems like a reasonable approach.
1 kΩ 15 mH Vm = 5 V ω = 50,000 rad/s EE 201 AC — the impedance way – 15 Working out the value for the voltage divider ratio: Plug in the numbers. Convert to magnitude/phase. Finish.
Then the resistor voltage is A sinusoid with amplitude of 4 V, shifted in phase by –36.9° from the source.
ZR ZR + ZL = R R + jωL = 1000 Ω 1000 Ω + j750 Ω = 1000 Ω (1250 Ω) e+j36.9∘ = (0.8) e−j36.9∘ vR = [(0.8) e−j36.9∘ ] [(5 V) exp (jωt)] vR = (4 V) ej(ωt −36.9∘) EE 201 AC — the impedance way – 16 Alternatively, we can use a math trick similar to Example 1: Divide top and bottom by R. Plug in the numbers Convert to magnitude/phase. Finish.
The final result would be the same. Note that the quantity ωL /R is dimensionless. (Check it.) ZR ZR + ZL = R R + jωL = 1 1 + j ωL R = 1 1 + j0.75 = 1 (1.25 ) e+j36.9∘ = (0.8) e−j36.9∘ EE 201 AC — the impedance way – 17 Time to drop the ejωt factor At the end of each of the previous examples, the answers were expressed as complex sinusoids, like . It should fairly obvious that every voltage and current in the circuit will have the factor ejωt built into it. The ejωt tells us that the quantity is oscillating with the angular frequency ω. Of course, we know that it will be oscillating at that frequency — the driving source sets up all the voltages and currents in the circuit. The source sets the pace and everything else must follow.
Since we know that all quantities will be multiplied by ejωt, there is really no need to include it at each step. All we really need is the magnitude and phase of the voltage or current. Writing the above answer as tells us everything we need to know. So from here on, we acknowledge that we know that everything is oscillating in the same manner, and we agree that we don’t need to attach ejωt everywhere. We know that is there implicitly, but we don’t need to write it explicitly.
So a voltage source can expressed more simply: . To help us remember that the quantities in the circuit are complex numbers representing sinusoids, we will add a little hat (tilde) over voltages or currents: or . (Looks like a tiny sine wave.) vR = (4 V) ej(ωt −36.9∘) vR = (4 V) e−j36.9∘ Vmej(ωt −0∘) →Vmej0∘→Vm ˜ VS = 10 V ˜ vR = (4 V) e−j36.9∘ EE 201 AC — the impedance way – 18 Example 3 Transform to the complex version of the circuit. (Use the new notation.) ZR = R ˜ iC = 1 ZC 1 ZR + 1 ZC ˜ IS Use AC analysis to find the capacitor current in the circuit below.
The theme of the day is dividers — use a current divider.
1 kΩ 0.1 µF Im = 25 mA ω = 7500 rad/s C R iC (t) iS (t) = Im cos (ωt) ZC ˜ IS = Im ZR ˜ iC ZC = 1 jωC EE 201 AC — the impedance way – 19 Working out the details for the current divider ratio: Plug in the numbers. (Ω–1 = S) Convert to magnitude/phase. Finish.
Then the complex capacitor current is The capacitor current will be a sinusoid oscillating with angular frequency ω = 7500 rad/s, having an amplitude of 15 mA and shifted in phase by 53.1° from the source.
1 ZC 1 ZR + 1 ZC = jωC 1 R + jωC = j0.75 mS 1 mS + j0.75 mS = (0.75 mS) e+j90∘ (1.25 mS) e+j36.9∘ = (0.6) e+j53.1∘ ˜ iC = [(0.6) ej53.1∘ ] (15 mA) = (25 mA) ej53.1∘ EE 201 AC — the impedance way – 20 Continuing with the math tricks, Divide top and bottom by jωC. Plug in the numbers Convert to magnitude/phase. Finish.
We should no longer be surprised that the result is the same.
1 ZC 1 ZR + 1 ZC = jωC 1 R + jωC = 1 1 + ( 1 jωRC) = 1 1 −j1.333 = 1 (1.667 ) e−j53.1∘ = (0.6) ej53.1∘ EE 201 AC — the impedance way – 21 Example 4 Transform to the complex version of the circuit.
ZR = R ˜ iR = 1 ZR 1 ZR + 1 ZL ˜ IS Use AC analysis to find the resistor current in the circuit below.
Ho Hum. Another day, another divider.
1 kΩ 0.015 H Im = 0.5 A ω = 66.7 krad/s ZL = jωL L R iR (t) iS (t) = Im cos (ωt) ZL ˜ IS = Im ZR ˜ iR EE 201 AC — the impedance way – 22 Looking at the current divider ratio: Plug in the numbers. (1/j = –j !) Convert to magnitude/phase. And done.
Then the complex resistor current is The resistor current is a sinusoid oscillating with angular frequency ω = 66,700 rad/s, having an amplitude of 0.354 A and shifted in phase by 45° from the source.
1 ZR 1 ZR + 1 ZL = 1 R 1 R + 1 jωL = 1 mS 1 mS −j1 mS = 1 mS (1.414 mS) e−j45∘ = (0.707) e+j45∘ ˜ iR = [(0.707) ej45∘ ] (0.5 A) = (0.354 A) ej45∘ EE 201 AC — the impedance way – 23 More math trickery, Multiply top and bottom by R. Plug in the numbers. Convert to magnitude/phase. Finish.
Yup.
1 ZR 1 ZR + 1 ZL = 1 R 1 R + 1 jωL = 1 1 + ( R jωL) = 1 1 −j1 = 1.414 (1.667 ) e−j45∘ = (0.707) ej45∘ EE 201 AC — the impedance way – 24 Example 5 Transform to the complex version of the circuit.
ZR = R ZL = jωL ˜ vC = ZC ZR + ZC + ZL ˜ VS It’s more fun when there are resistors, capacitors, and inductors all together. Find the important sinusoid information about the capacitor voltage in the circuit. It’s hard to avoid voltage dividers.
1 kΩ 15 mH Vm = 5 V ω = 40,000 rad/s 100 nF + – R C – + vC (t) vS (t) = Vm cos (ωt) L + – – + ZR ZC ZL ZC = 1 jωC ˜ vC ˜ VS = Vm EE 201 AC — the impedance way – 25 Plug in the numbers. Combine. Convert. Finish.
Then the complex capacitor voltage is A sinusoid with amplitude of 1.18 V, shifted in phase by –109.3° from the source.
ZC ZR + ZC + ZL = 1 jωC R + 1 jωC + jωL = −j250 Ω 1000 Ω −j250 Ω + j600 Ω = −j250 Ω 1000 Ω + j350 Ω = (250 Ω) e−j90∘ (1060 Ω) e+j19.3∘ = (0.236) e−j109.3∘ ˜ vR = [(0.236) e−j109.3∘ ] (5 V) = (1.18 V) e−j109.3∘ EE 201 AC — the impedance way – 26 There are some manipulations we can apply here as well. Multiply top/bottom by jωC. Re-arrange. Plug in the numbers Convert. Finish.
Note yet another dimensionless quantity: . (Check this, too.) ZC ZR + ZC + ZL = 1 jωC R + 1 jωC + jωL = 1 jωRC + 1 −ω2LC = 1 (1 −ω2LC) + j (ωRC) = 1 −1.4 + j4 = 1 (4.24 ) e+j109.3∘ = (0.236) e−j109.3∘ ω2LC EE 201 AC — the impedance way – 27 Example 6 Transform to the complex version of the circuit.
ZR = R ˜ iC = 1 ZC 1 ZR + 1 ZC + 1 ZL ˜ IS We should do an RLC current divider — it wouldn’t be right to ignore it. Find the capacitor current.
We know how this goes.
100 Ω 0.1 µF Im = 100 mA ω = 66.7 krad/s ZC = 1 jωC L R iS (t) = Im cos (ωt) C iC (t) 15 mH ZC ZR ZL ZL = jωL ˜ iC ˜ IS = Im EE 201 AC — the impedance way – 28 Plug in the numbers. Combine. Convert. Finish.
Then the complex capacitor current is We know what this means. We will skip the alternate math here, but you should try a math trick for yourself. (Multiply by jωL or divide by jωC.) 1 ZC 1 ZR + 1 ZC + 1 ZL = jωC 1 R + jωC + 1 jωL = j6.67 mS 10 mS + j6.67 mS −j1 mS = j6.67 mS 10 mS + j5.67 mS = (6.67 mS) e+j90∘ (11.5 mS) e+j29.6∘ = (0.58) e+j60.4∘ ˜ iC = [(0.58) ej60.4∘ ] (100 mA) = (58 mA) ej60.4∘ EE 201 AC — the impedance way – 29 Z1 = R1 = (R2) ( 1 jωC) R2 + 1 jωC 1 kΩ 0.1 µF Vm = 10 V ω = 20,000 rad/s Example 7 Let’s try this circuit— it looks a bit like the RC circuit from example 1. Find the voltage across the parallel combination of R2 and C.
1 kΩ + – C – + v2 (t) vS (t) = Vm cos (ωt) R1 R2 + – – + Z1 Z2 In fact, this is yet another simple voltage divider, if we treat the R2-C combination as a single impedance.
˜ v2 ˜ VS = Vm Z2 = ZR2 ZC = R2 ( 1 jωC ) = R2 1 + jωR2C ˜ v2 = Z2 Z1 + Z2 ˜ VS EE 201 AC — the impedance way – 30 Inserting the impedances into the voltage divider expression : Yikes! That looks messy. At this point in previous examples, we were able to substitute values directly and do the complex calculations without too much hassle. In this case, if we substitute values now, there will be many conversions back and forth between real-imaginary and magnitude-phase — the math will be quite tedious and prone to errors. In the earlier examples, we also showed that a bit of algebraic manipulation could make the math a bit cleaner, although the extra steps were not really necessary in those simpler problems. However, in this example, some algebraic manipulation is not just advisable, it is probably necessary in order to make the ensuing math tenable. To simplify this expression, we can multiply top and bottom by 1 + jωR2C: That’s nicer. Inserting values. Not bad at all.
Z2 Z1 + Z2 = R2 1 + jωR2C R1 + R2 1 + jωR2C Z2 Z1 + Z2 = R2 R1 + R2 + jωR1R2C = 1000 Ω 2000 Ω + j2000 Ω EE 201 AC — the impedance way – 31 Continuing with voltage divider ratio: Convert to magnitude/phase. Finish. Then the complex voltage across the parallel combination is There is one additional algebra step we might have tried before inserting values. If, after the first simplification, we divide top and bottom by R1+R2, the divider expression becomes: The extra step is not essential, but it does offer some insights.
Z2 Z1 + Z2 = 1000 Ω 2000 Ω + j2000 = 1000 Ω (2828 Ω) e+j45∘ = (0.354) e−j45∘ ˜ v2 = [(0.354) e−j45∘ ] (10 V) = (3.54 V) e−j45∘ R2 R1 + R2 1 + jω ( R1R2 R1 + R2) C = 0.5 1 + j1 = 0.5 2ej45∘= 0.354e−j45∘ EE 201 AC — the impedance way – 32 Z2 = R2 1 kΩ 15 mH Im = 50 mA ω = 50,000 rad/s Example 8 One more divider — find the key features of the sinusoidal current iR2.
Again, we have a simple current divider if we treat the R1-L series combination as a single impedance.
˜ i2 ˜ IS = Im Z1 = ZR1 + ZL = R1 + jωL ˜ i2 = 1 Z2 1 Z1 + 1 Z2 ˜ IS 1 kΩ Z2 Z1 L iR2 (t) iS (t) = Im cos (ωt) R1 R2 EE 201 AC — the impedance way – 33 Inserting the impedances into the voltage divider expression: This could use some tidying up before inserting numbers. Multiply top and bottom by R1 + jωL: That’s better. Inserting values — nice and clean. Then the complex current through R2 is 1 Z2 1 Z1 + 1 Z2 = 1 R2 1 R1 + jωL + 1 R2 = R1 R2 + j ( ωL R2 ) 1 + R1 R2 + j ( ωL R2 ) = 1 + j0.75 2 + j0.75 = (1.25) ej36.9∘ (2.136) ej20.6∘= (0.585) ej16.3∘ ˜ i2 = [(0.585) ej16.3∘ ] (50 mA) = (29.25 mA) ej16.3∘ EE 201 AC — the impedance way – 34 1 kΩ 10 nF Vm = 0.5 V ω = 8330 rad/s Example 9 Let’s try an op amp. Find the important information (magnitude, phase) for the sinusoidal output voltage. (Not a divider! Woo Hoo!) How do ops amp work in a complex circuit? Just like they did before. The rules are unchanged: no current flows into the input, , and when there is a negative feedback loop, . If we treat the resistor/capacitor parallel combination as a single impedance, the complex version of the circuit has the form of a simple inverting amp.
˜ i+ = ˜ i−= 0 ˜ v+ = ˜ v− ˜ vS = Vm G = ˜ vo ˜ vs = −Z2 Z1 12 kΩ – + R1 R2 C vS (t) = Vm cos (ωt) vS (t) vo (t) – + Z1 Z2 Z2 = ZR2 ZC = R2 1 + jωR2C Z1 = R1 ˜ vo (As seen previously.) EE 201 AC — the impedance way – 35 With a tiny bit of re-arrangement: Inserting values Transform to polar. Watch the negative sign! Then the complex output voltage is Op amps are so easy.
G = −Z2 Z1 = − R2 1 + jωR2C R1 = − R2 R1 1 + jωR2C = −12 1 + j1 = (12) ej180∘ (1.414) ej45∘ = (8.49) ej135∘ ˜ vo = G ⋅˜ vS = [(8.49) ej135∘ ] (0.5 V) = (4.24 V) ej135∘ EE 201 AC — the impedance way – 36 1 kΩ 10 uF Vm = 0.5 V ω = 100 rad/s Example 10 Op amps are fun. Let’s do one more. Find the complex output voltage for the non-inverting amp at right.
It may not be immediately obvious that this is a non-inverting amp, but if we treat the R1-C series combination as a single impedance, we can draw the complex version of the circuit. Then it is familiar.
˜ vS = Vm G = ˜ vo ˜ vs = 1 + Z2 Z1 22 kΩ vS (t) = Vm cos (ωt) vS (t) vo (t) Z1 = ZR1 + ZC = R1 + 1 jωC Z2 = R2 ˜ vo – + R2 R1 C – + Z2 Z1 The complex expression for the gain of non-inverting amp would be: EE 201 AC — the impedance way – 37 Proceed with caution. It is easy to jump to wrong conclusions. Insert values Transform to polar and finish.
Then the complex output voltage is G = 1 + Z2 Z1 = 1 + R2 R1 + 1 jωC = R1 + 1 jωC R1 + 1 jωC + R2 R1 + 1 jωC = R1 + R2 −j ( 1 ωC ) R1 −j ( 1 ωC) = 23000 Ω −j1000 Ω 1000 Ω −j1000 Ω = (23002 Ω) e−j2.5∘ (1414 Ω) e−j45∘= 16.27e−j42.5∘ ˜ vo = G ⋅˜ vS = [(16.3) ej42.4∘ ] (0.5 V) = (8.13 V) ej42.5∘ EE 201 AC — the impedance way – 38 This is an example where an extra math step leads to an instructive result. Starting at the step where Divide top and bottom by R1. Note how 1 + R2/R1 appears. G = R1 + R2 −j ( 1 ωC) R1 −j ( 1 ωC) = R1 + R2 R1 −j ( 1 ωR1C) 1 −j ( 1 ωR1C ) = (1 + R2 R1 ) −j ( 1 ωR1C) 1 −j ( 1 ωR1C) = 23 −j1 1 −j1 = (23.02) e−j2.5∘ (1.414) e−j45∘= (16.3) ej42.5∘ |
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When writing log, do you indicate the base, even when 10?
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Ive been working with many students on logarithms and have noted that log has a base of 10 unless specified. Further, I commented that putting a 10 as a subscript to log is redundant, or at least not needed. A student sent me this, from a popular math blog. Now I am wondering if I made a mistake. This image basically implies when using log, always indicate the base, to avoid confusion.
Edit: When this came to my attention, I was reminded of a prior question "Why do we write ð¥ instead of 1ð¥ ?" It seems from the replies, this is a different situation.
secondary-education
logarithm
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edited Mar 17, 2023 at 10:37
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asked Mar 16, 2023 at 18:25
JTP - Apologise to MonicaJTP - Apologise to Monica
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$\begingroup$ I think using $\log$ to mean both $\log_{10}$ and $\log_e$ is pretty common. The usual solution is to just announce your convention once the first time you use it in a paper. I would recommend this practice for students as well. $\endgroup$
Steven Gubkin
– Steven Gubkin
2023-03-16 18:37:27 +00:00
Commented Mar 16, 2023 at 18:37
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$\begingroup$ It seems reasonable to me to match what the calculators say. I think that's least confusing. $\endgroup$
Sue VanHattum
– Sue VanHattum ♦
2023-03-17 03:12:49 +00:00
Commented Mar 17, 2023 at 3:12
4
$\begingroup$ IMO, use $log10$, $ln$, $log2$, $log_b$ (b is the base) to specify a logarithm and $log$ when the base is irrelevant. $\endgroup$
chux
– chux
2023-03-17 09:12:57 +00:00
Commented Mar 17, 2023 at 9:12
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$\begingroup$ As with all high-school topics: follow the textbook. Do not introduce your own notation differing from the textbook. NOTE. $\endgroup$
Gerald Edgar
– Gerald Edgar
2023-03-17 09:23:10 +00:00
Commented Mar 17, 2023 at 9:23
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$\begingroup$ I would also add Computer Scientist thinks $\log_2(50)$ to the slide. If I recall well, I used to denote $\log_2$ with $\text{lg}$, so you might want to add that. For high school I believe it is absolutely necessary to differentiate the cases. However at higher levels, writing the basis is redundant, as the most important property of logarithm is independent of the basis, and it is usually understood from the context (or mentioned once in the beginning of book/article/...). $\endgroup$
Kolja
– Kolja
2023-03-17 18:55:22 +00:00
Commented Mar 17, 2023 at 18:55
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5 Answers 5
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And a computer scientist thinks that $\log=\log_2$. I am using $\log$ for the natural logarithm by default in all my courses though I clearly state that in the beginning of each course (I teach at the university level). In general, one can use any default base one wishes provided that it has been made clear what it is and that the usage is consistent. At the school level the common tradition is to use $\log$ for base $10$ and $\ln$ for natural logarithm, but if you go higher and look at various textbooks in STEM subjects, both old and modern, this convention is rarely upheld there.
So, my advice is rather to alert the students that $\log$ without base indicated may mean different bases in different contexts and, if the base is not immediately clear, the clarification should be sought and/or requested.
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answered Mar 16, 2023 at 18:45
fedjafedja
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$\begingroup$ One has to be careful with computer language functions as well... $\endgroup$
Jon Custer
– Jon Custer
2023-03-16 18:54:43 +00:00
Commented Mar 16, 2023 at 18:54
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$\begingroup$ I vaguely recall seeing lg mean "log base 2" in some programing language/library once. "Always clarify avoids confusion" is the right answer. $\endgroup$
SkySpiral7
– SkySpiral7
2023-03-17 21:51:54 +00:00
Commented Mar 17, 2023 at 21:51
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$\begingroup$ As a 40-year computer programmer I've never thought that log=log2. $\endgroup$
Barmar
– Barmar
2023-03-18 13:35:38 +00:00
Commented Mar 18, 2023 at 13:35
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$\begingroup$ I've generally seen log-base-2 writte as lg, to distinguish it from log-base-10 log, and log-base-e ln. $\endgroup$
supercat
– supercat
2023-03-18 19:47:32 +00:00
Commented Mar 18, 2023 at 19:47
1
$\begingroup$ @supercat - That seems to conflict with this answer from cbeleites (and the comments under that answer), where lg => log-base-10. $\endgroup$
Greenonline
– Greenonline
2023-03-19 01:41:42 +00:00
Commented Mar 19, 2023 at 1:41
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I'm in Germany (chemist, FWIW). I'm familiar with:
$\log$: base is unknown/not needed (as in $\log (a) + \log (b) = \log (ab)$
natural logarithm: $\ln = \log_e$
base 10 logarithm: $\lg = \log_{10}$
In chemistry, both natural and base 10 logarithm are used a lot: The natural logarithm wherever one has to differentiate or integrate (naturally ;-) ), e.g. in kinetics or statistical thermodynamics. In parallel, base 10 logarithm is used a lot in definitions of physical quantities like $\mathrm{pH}$, $\mathrm{pK}_a$, absorbance etc. In some cases (e.g. Beer-Lambert-law) there is some ambiguity and field-dependent definitions. In that case, we sometimes include the base in the name of the quantity, e.g. the decadic molar absorption coefficent.
$\mathrm{lb} = \log_2$ Rare. I've seen it and I recognize it - but I'd spell out this definition rather than assuming any reader to be familiar with this. Don't know whether one could assume computer scientists to be familiar with this.
Update: From this answer on math.sx I learned that this notation is ISO standard.
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edited Mar 17, 2023 at 12:29
answered Mar 17, 2023 at 8:03
cbeleitescbeleites
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$\begingroup$ In CS, we defined $ld = log_2$ (d for dualis) $\endgroup$
Luatic
– Luatic
2023-03-17 09:13:08 +00:00
Commented Mar 17, 2023 at 9:13
3
$\begingroup$ I'm familiar with lg=log (and of course ln=log) in the UK (physics/engineering) usage too. Any others are rare and specified. The times we have to check are calculators and software using "log" without stating the base (Mate calculator on Linux has buttons for ln and log; you can override the base on the latter, but nowhere does it state that the default is 10) $\endgroup$
Chris H
– Chris H
2023-03-17 13:56:55 +00:00
Commented Mar 17, 2023 at 13:56
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$\begingroup$ Ah yes lb. For when you want the result to be in pounds. $\endgroup$
SkySpiral7
– SkySpiral7
2023-03-17 21:53:30 +00:00
Commented Mar 17, 2023 at 21:53
3
$\begingroup$ $\mathrm{lb}$ is an ISO standard, though that's literally the only reason I know about it. I've never seen it used. $\endgroup$
chepner
– chepner
2023-03-17 23:07:28 +00:00
Commented Mar 17, 2023 at 23:07
$\begingroup$ (And of course log(ð)+log(ð)=log(ðð) is only true if all three logarithms use the same base so it may be better to specify it e.g. as ð.) $\endgroup$
gidds
– gidds
2023-03-17 23:20:03 +00:00
Commented Mar 17, 2023 at 23:20
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I think stereotypically that log means base 10 and ln means base e. That is how all the 8 different high school and college texts (published 30s to 80s) that I have use it. But I have noticed a (maybe growing?) tendency for other usage. Had to get a formal paper in econ to define their base. (And they were using the log means base e usage, that is more rare...at least for knuckle draggers like me.)
I did a quick Google search on does log mean log base 10 and their were several university math tutor sites still propounding the orthodox religion about common logs. But, a few heretics were seen also. :-(
"So, when you see log by itself, it means base ten log. When you see ln, it means natural logarithm (we'll define natural logarithms below). In this course only base ten and natural logarithms will be used."
U Minn:
My advice would be to stick with the log means 10 usage since it is still (I think) the most common usage and it's your class that they mostly need it in. I still remember fondly log tables (base 10) being handed out for AP chem into the 90s, in case kids did not have a calculator. ;-)
Maybe briefly mention it to the kids, that some usage is different. (heck "billion" means something different in different countries...and don't get me started on the comma/decimal hassles when passing documents back and forth with Germans).
I wouldn't feel too worried if they see something different in the future. That can be dealt with then by the other teacher. Or if they are really doing sophisticated work in econ or pure math, than they'll be quite capable of dealing with the momentary notation confusion.
Also, FWIW, I wouldn't worry about alternate usage in the more rarified air of higher math courses. Most of your kids need to learn things the old school way and they will be heading for the natural sciences or engineering (which are more traditional). If they end up reading a measure theory text, there's other parts of the text that will vex them more than Napierian being treated as common. ;)
P.s. Of course if you're tutoring and you learn the teach has other usage, defer to him. Or her. Or it.
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edited Mar 16, 2023 at 19:00
answered Mar 16, 2023 at 18:52
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Partially tongue in cheek, but it would feed two birds with one apple :
"Henceforth this book | article | thesis uses the following notation
$ ln( \sqrt {-1} ) = \frac \pi 2 i $
() or
$ log_e( \sqrt {-1} ) = \frac \pi 2 i $
() or
$ Log_{2}( 1 T_i ) = 40 $
() or
$ log( \sqrt {-1} ) = \frac \pi 2 j $
() or
$ log( \sqrt {-1} ) = \frac \pi 2 i $ "
() - only one used
Then we'd know if we're in the good company of mathematicians, scientists, computer scientists, electrical engineers or all other engineers.
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answered Mar 19, 2023 at 18:57
Nick MyraNick Myra
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$\begingroup$ Would you mind editing your answer to make it less tongue-in-cheek? That'd make it more useful to anyone reading it. $\endgroup$
Joonas Ilmavirta
– Joonas Ilmavirta
2023-03-19 19:30:23 +00:00
Commented Mar 19, 2023 at 19:30
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My experience as university student, researcher and teacher in technical and scientific fields in Italy has taught me that the only widely known unambiguous notation is:
ln(x) for base e log (most common)
Log(x) for base 10 log (slightly less common note the capital "L"), but probably to be avoided when writing things by hand, since the capitals can be easily be warped by quick handwriting.
The notation log(x) (sometimes abbreviated as lg(x) in Italy) is used to indicate mostly natural logarithm (especially in math courses), but also frequently base 10 logarithm (in some engineering courses, for example). Some computer scientists use it to indicate base 2 log, but it is far less common (but not at all rare).
What my math professors at university always said was to check my assumptions when using the "baseless" notation and to check any paper/book that used that notation for disambiguation clues, such as symbol lists, because there was no universal standard or practice to rely on.
The only important thing is to be consistent: if you choose to use "log" for natural logarithms, then state so upfront, remind that choice often to your students (especially at the beginning), point out that it is not an universal choice, and never, ever, use that symbol for something else in the same context or with the same group of students.
My usual choice nowadays (in technical fields) is to use log for base 10 (so I don't have capitalization issues) and ln for base e, so it matches any pocket calculator a student may be using.
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edited Mar 20, 2023 at 11:03
answered Mar 19, 2023 at 11:56
LorenzoDonati4Ukraine-OnStrikeLorenzoDonati4Ukraine-OnStrike
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$\begingroup$ Gosh, $\ln(x)$ means base $2,$ $\lg(x)$ means base $e,$ and the capital 'L' in $\operatorname{Log}(x)$ signifies base $10 ?$ These are indeed far removed from all corners of mathematical practice. $\endgroup$
ryang
– ryang
2023-03-19 14:29:39 +00:00
Commented Mar 19, 2023 at 14:29
1
$\begingroup$ and in other contexts, "Log(z)" with the uppercase L is used for the main branch of the complex logarithm, where the general log(z) would be multi-valued... $\endgroup$
ilkkachu
– ilkkachu
2023-03-19 18:43:27 +00:00
Commented Mar 19, 2023 at 18:43
$\begingroup$ @ryang Sorry, I didn't recheck my post. I a dumb typo crept in at the beginning (as my last sentence could have hinted). See my correction. $\endgroup$
LorenzoDonati4Ukraine-OnStrike
– LorenzoDonati4Ukraine-OnStrike
2023-03-20 11:03:00 +00:00
Commented Mar 20, 2023 at 11:03
$\begingroup$ Haha ok, noted. Thats perhaps why your post got downvoted (not from me though). -( $\endgroup$
ryang
– ryang
2023-03-20 11:06:32 +00:00
Commented Mar 20, 2023 at 11:06
1
$\begingroup$ @ryang BTW, thanks for the comment. Without it the post could have been rightfully downvoted to oblivion! :-) $\endgroup$
LorenzoDonati4Ukraine-OnStrike
– LorenzoDonati4Ukraine-OnStrike
2023-03-20 11:10:17 +00:00
Commented Mar 20, 2023 at 11:10
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11357 | https://www.youtube.com/watch?v=KeiRNueSXEY | How to use a scientific calculator to Find Powers and Exponents on a Calculator|Math Defined
Math Defined
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Posted: 6 May 2022
Hello! Welcome to "How to use a scientific calculator to Find Powers and Exponents on a Calculator" by Math Defined with Mrs. C.
Do you need to learn how to use a Texas Instruments Scientific calculator to find the values of powers and exponents? Whether you need a detailed explanation or just a quick refresher, this video is for you!
In this video, I will guide you through four exponents problems. I will show you the specific keys on the calculator that you need to use in order to enter the exponents. I show you examples of exponents that are positive, negative and in fraction form.
I I hope you enjoy this video and that it helps you to be able to use your scientific calculator to easily find the values of powers and exponents!
Here is the link to the calculator that I used in this video -
This video is not sponsored. Some links are affiliated links which means that as an Amazon Associate I earn a small commission from qualifying purchases.
About Math Defined with Mrs. C. This channel provides instructional math videos that are directly aligned with math standards. Students, teachers, and parents/guardians from around the world have used these videos to help teach math skills and content.
Do you need a math tutor with a certified math teacher? Math Defined offers online math tutoring. For more information email me at mathdefined.com adding and subtracting fractions
29 comments
Transcript:
Do you want to know a super easy way to use your
calculator to find powers and exponents? Well, if you do, you are in the right place! This is
Math Defined and I'm Mrs. C. and I'm going to show you the easy way to find powers on this scientific
calculator. Before I begin solving those problems that are listed to the left of my calculator here,
I do want to go over four specific buttons that we will be using on this scientific calculator. So
besides all the white buttons here that are just our number buttons, we will be using the button
that looks right here that looks like x squared. We will be using this button here that looks
like a carrot. We will be using this button right here that looks like a mixed number or the
A b/c button. And, we will be using this button down here that looks like a minus button. So let's
get started. We're going to start by looking at our first example of 3 squared. Now this is a
power and if you recall from my previous video on Powers and Exponents, powers have two components.
They have a base and they have an exponent. And the base is the large number and the exponent
is the small number that is on the right side or actually the upper right side of the base. So when
you are putting these powers into your calculator, you always put the base in first. So, I'm going to
go ahead and clear my calculator and I'm going to do my first example of three squared. So, three is
my base so I"m going to go ahead and put my three in, and for this particular one since my exponent
is a two I'm going to use this button right here because this looks like x to the power of 2 and
in this case x can be any number and I have a three for my number at this time so I'm going
to ahead click this button here and do you see up here is says three squared. So this is
three to the second power or three squared then I come down here and hit my equal or my
enter button so I know that three squared is equal to 9. And remember to find that, you can do
that mentally actually because three squared is just three times three and three times three is 9.
Now I'm going to clear this. Now my next example is three to the fifth. And as you can see three to
the fifth is equal to a much larger number than 9 and that is 243. So now we're really happy that
we have a calculator to help us with this one. So three is my base so I put that in first.
Now I can not use this button here because this is the button that is used when your
exponent is a 2 while my exponent is a 5. So that means that I am going to come up
here to this button that looks like a carrot but it's actually an exponent button. And whether
you're using a Texas Instruments scientific calculator or any of the other brands that are out
there that are just as good as a Texas Instrument, usually the buttons are pretty much universal or
the the same. So when you see something like this, this is going to be your exponent button. So
I went ahead and I clicked the exponent button and my exponent is a 5 and then I go ahead
hit my equals or my enter and there I get 243. Isn't this easy? So now I'm going to do
another one that looks kind of challenging! Now I have a power that is 4 to the 1/2.
So I'm going to clear this and again your base always goes in first. So I"m going to
put my 4 in and I don't have an exponent of 2 so I need to go up here to my carrot button
because my exponent is something other than 2, but now my exponent is a fraction of 1/2. So,
I'm going to use this fraction button to help me create that fraction of 1/2. So, the first
thing I do is I put my 1 for my numerator here, then I go to my fraction button and then I put the
denominator of 2. So this little backwards L here is the fraction bar separating the numerator
from the denominator. And then all I have to do is come down here and hit enter. And
so 4 to the 1/2 power is 2. Now one more. This time I have 10 to the negative 2 power.
So again we are going to start by putting our base in first. Now this is a 2 as well as
my 10 to the 2 but that is a negative 2, not a positive 2 and this button you use
when you have a positive exponent of 2. And I don't have a positive exponent of
2, so I need to use my exponent button. Now I also want to show you here, if you
are new to using these kinds of calculators, a very common mistake that people make is when
they see the negative numbers like negative 2, they go ahead and they use this minus sign right
here to show a negative number. So let me show you what happens if you do that. So let's go ahead
and put this button here, then our exponent of 2 and so now I'm going ahead and hit my enter
and you see that I get a Syntax Error? And sometimes when people especially when
they are new to using this calculator they think oh, well this calculator can't
do negative exponents. And that is just not correct at all because it really can, you
just have to know the correct buttons to use. So let's clear it and clear it all the way. I'm
going to put my base of 10, go ahead and hit my exponent button. Now the correct negative
sign button on this scientific calculator is this one right here. So whenever you have a
negative number, this is what you going to click not the minus sign because this is subtract,
this doesn't mean negative it means subtract. So I need to click this button here and then my 2.
And if you'll notice, if you back up on the video you'll notice that is negative sign here looks
a little bit different than the subtraction sign did when we did it before. So now I'm ready
to hit enter and I get an answer of 0.01. And that's all there is to it. Now you have
it! Well I hope that this video was helpful to you and and if it was please let me know
by becoming a subscriber today and leave me a comment in the comments section below. So until I
see you next time, thank you so much for watching. |
11358 | https://learninglab.rmit.edu.au/maths-statistics/algebra/algebra-getting-started/a21-rearranging-formulae/ | RMIT University
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Transposing formulas
The transposition of formulas involves rearranging equations to solve for a specific pronumeral or variable. You need to be able to first isolate your desired variable in order to solve problems various fields. Mastering transposition will enhance your ability to manipulate and understand mathematical relationships effectively.
Video tutorial – transposition of formulas
Watch this video to learn about the transposition of formulas.
Formulas
Formulas set out the mathematical relationships between variables. You may have learned that you can easily substitute numbers or values into formulas to find an unknown.
Examples include:
(A=\pi r^{2})
(s=ut+\dfrac{1}{2}at^{2})
(S=P(1+i)^{n})
In these examples, (A), (s) and (S) are the subjects of the formulas. A subject is shown on one side of the equal sign of the formula, followed by an equal sign.
Transposing formulas
Sometimes, a formula is given in a particular form and you need to rearrange it to make a different variable the subject.
For example, you might know the area of a circle ((A)) and want to find the radius ((r)). It is perfectly reasonable to substitute the area into the formula (A=\pi r^{2}), but making (r) the subject will make problem-solving much more efficient.
To transpose formulas, we need to "undo" the operations to make a different variable the subject of the formula. You do this by doing the opposite operation. The following table tells you what you need to do to undo certain operations.
| Operation | Opposite operation |
--- |
| subtraction ((-)) | addition ((+)) |
| multiplication ((\times)) | division ((\div)) |
| square root ((\sqrt{x})) | square ((x^{2})) |
Note that when taking the square root of a term—let's say, (x^{2})—the answer will be (\pm x). This is because (x\times x=x^{2}) but also ((-x)\times(-x)=x^{2}). Since we may not know whether the (x) is positive or negative, we must indicate that (\sqrt{x^{2}}=\pm x).
There is a basic rule you can follow to transpose formulas:
When rearranging equations and formulas, whatever you do on one side of the equal sign, you must do on the other.
When you encounter questions asking you to transpose a formula, you may see the terms "rearrange", "transform", "make (x) the subject", or "express in terms of (x)". These are all instructions transpose formulas.
Example 1 – transposing formulas
Make (A) the subject in the formula (A+B=C).
We need to undo the operations to get (A) on its own on one side of the equal sign. On the left, (B) is added to (A), so we can remove it by subtracting (B) on both sides.
[\begin{align} A+B & = C\quad\textrm{subtract (B) from both sides}\A+B-B & = C-B\A & = C-B\end{align}]
Make (A) the subject in the formula (AB=C).
We need to undo the operations to get (A) on its own on one side of the equal sign. On the left, (B) is multiplied by (A), so we can remove it by dividing by (B) on both sides.
[\begin{align} AB & = C\quad\textrm{divide both sides by (B)}\\frac{AB}{B} & = \frac{C}{B}\quad\textrm{cancel out (B) on left}\A & = \frac{C}{B}\end{align}]
Make (A) the subject in the formula (A^{2}=B).
We need to undo the operations to get (A) on its own on one side of the equal sign. On the left, (A) is squared, so we can remove the square by taking the square root of both sides.
[\begin{align} A^{2} & = B\quad\textrm{take square root of both sides}\\sqrt{A^{2}} & = \pm\sqrt{B}\A & = \pm\sqrt{B}\end{align}]
Transform (V=A-K) to make (A) the subject.
We need to undo the operations to get (A) on its own on one side of the equal sign. On the right, (K) is subtracted from (A), so we can remove it by adding (K) to both sides.
[\begin{align} V & = A-K\quad\textrm{add (K) to both sides}\V+K & = A-K+K\V+K & = A\end{align}]
We can rewrite this so that (A) is on the left.
[A=V+K]
Make (d) the subject of (C=\pi d).
We need to undo the operations to get (d) on its own on one side of the equal sign. On the right, (d) is multiplied by (\pi), so we can remove it by dividing by (\pi) on both sides.
[\begin{align} C & =\pi d\quad\textrm{divide by (\pi) on both sides}\\frac{C}{\pi} & = \frac{\pi d}{\pi}\quad\textrm{cancel out (\pi) on right}\\frac{C}{\pi} & = d\end{align}]
We can rewrite this so that (d) is on the left.
[d=\frac{C}{\pi}]
Rearrange (j=3w-5) in terms of (w).
We need to undo the operations to get (w) on its own on one side of the equal sign. On the left, (w) is multiplied by (3), then (5) is added. To undo this, we need to work backwards and subtract the (5) first, then divide by (3).
[\begin{align} j & = 3w-5\quad\textrm{add (5) on both sides}\j+5 & = 3w-5+5\j+5 & = 3w\quad\textrm{divide by (3) on both sides}\\frac{j+5}{3} & = \frac{3w}{3}\quad\textrm{cancel out (3) on right}\\frac{j+5}{3} & = w\end{align}]
We can rewrite this so that (w) is on the left.
[w=\frac{j+5}{3}]
Make (c) the subject of (E=mc^{2}).
We need to undo the operations to get (c) on its own on one side of the equal sign. On the left, (c) is squared and multiplied by (m). To undo this, we need to work backwards and divide by (m) first, then take the square root.
[\begin{align} E & = mc^{2}\quad\textrm{divide by (m) on both sides}\\frac{E}{m} & = c^{2}\quad\textrm{take square root of both sides}\\sqrt{\frac{E}{m}} & = \sqrt{c^{2}}\\sqrt{\frac{E}{m}} & = c\end{align}]
We can rewrite this so that (c) is on the left.
[c=\sqrt{\frac{E}{m}}]
Exercise – transposing formulas
Find (n) if (m=n-2).
Find (C) if (A=2B+C).
Find (B) if (A=2B+C).
Find (k) if (P=\dfrac{k}{V}).
Find (V) if (PV=k).
Find (a) if (v=u+at).
Find (t) if (v=u+at).
Find (A) if (r=\sqrt{\dfrac{A}{\pi}}).
Find (x) if (A=x^{2}).
Find (r) if (A=\pi r^{2}).
(n=m+2)
(C=A-2B)
(B=\dfrac{A-C}{2})
(k=PV)
(V=\dfrac{k}{P})
(a=\dfrac{v-u}{t})
(t=\dfrac{v-u}{a})
(A=\pi r^{2})
(x=\pm\sqrt{A})
(r=\pm\sqrt{\frac{A}{\pi}})
Images on this page by RMIT, licensed under CC BY-NC 4.0
Keywords
Algebra
Arithmetic
Functions
Maths equations
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2025 AIME I Problems/Problem 8
Contents
1 Problem
2 Video solution by grogg007
3 Solution 1
4 Solution 2 (Systematic + Algebra)
5 Solution 3 (A Little Geometry)
6 Solution 4 (Distance Formula, quick)
7 See also
Problem
Let be a real number such that the system |25+20 i−z|=5|z−4−k|=|z−3 i−k| has exactly one complex solution . The sum of all possible values of can be written as , where and are relatively prime positive integers. Find . Here .
Video solution by grogg007
Solution 1
The complex number must satisfy the following conditions on the complex plane:
The magnitude between and is This can be represented by drawing a circle with center and radius
It is equidistant from the points and Hence it must lie on the perpendicular bisector of the line connecting these points.
For to have one solution, the perpendicular bisector of the segment connecting the two points must be tangent to the circle. This bisector must pass the midpoint, and have slope The segment connecting the point of tangency to the center of the circle has slope meaning the points of tangency can be or Solving the equation for the slope of the perpendicular bisector gives or giving or , having a sum of
~nevergonnagiveup
Solution 2 (Systematic + Algebra)
We first look at each equation, and we convert each to algebra (note that the absolute value sign of means the magnitude). Let's convert z to .
Note that the first equation becomes:
Note that this is the equation of a circle centered at with radius .
And the second equation becomes:
You can see that the many similar terms that cancel out, simplfying, you get:
Now we must isolate B
This equation can be seen as a line with a slope, and a y-intercept of .
Note that the question only wants one solution, so we want two tangent lines, one above the circle, and one below the circle. You can see Solution 2 for the picture.
Because the slope is , the circle must have a slope coming out of center of its reciprocal, . So the points on the circle where this line with a must intersect must be and . We can easily use point-slope form to find the equations of these lines.
and
Now we must match the y-intercepts to the equations with in it. Solving the equations:
we get that and Adding them up and simplifying, we get a sum of
~Marcus:)
Solution 3 (A Little Geometry)
To solve the problem, we first locate the point . According to the conditions, we can know that:
is on the perpendicular bisector of and
The distance from to circle is .
Therefore, must be the 2 points of tangent of a line with the slope of with circle O (center at , radius of ), corresponding to the 2 values: and .
Since the question only asks for the sum of and , we would not need to calculate them separately. Let the middle point of and be ==> + = .
Looking at the simplified figure below. We may calculate using similarity of the triangles:
We conclude that .
~cassphe
Solution 4 (Distance Formula, quick)
Let Then the system becomes and . For this system to have one solution for the line must be tangent to the circle . For a line to be tangent to a circle, the distance between the line and center must be equal to the length of the radius, which is . The center of the circle is and we can express the line as So we have: is The requested sum is
~grogg007, Mathycoder & MathKing555 also previously mentioned a similar approach
See also
2025 AIME I (Problems • Answer Key • Resources)
Preceded by
Problem 7Followed by
Problem 9
1•2•3•4•5•6•7•8•9•10•11•12•13•14•15
All AIME Problems and Solutions
These problems are copyrighted © by the Mathematical Association of America, as part of the American Mathematics Competitions.
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11360 | https://goopenct.org/courseware/lesson/1053/student/?section=15 | Connecticut Model Math for Grade 6, Algebraic Reasoning, Unit 6 Overview: Algebraic Reasoning | GoOpen CT
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Connecticut Model Math for Grade 6
Algebraic Reasoning
Operating with Positive Rational Numbers
Understanding Positive and Negative Numbers
Using Expressions and Equations
Applications of Geometry
Ratios and Rates
Algebraic Reasoning
Statistics and Distributions
Unit 6 Overview: Algebraic Reasoning
Unit 6 Overview: Algebraic Reasoning
Unit 6 Overview: Algebraic Reasoning
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Title
1 - Relevant Standards:
2 - Examples and Explanations:
3 - Transfer Goal: Aligned to district portrait or vision of the learner
4 - Essential Questions:
5 - Enduring Understanding:
6 - What Students Will Know:
7 - What Students Will Do:
8 - Demonstration of Learning:
9 - Unit Specific Vocabulary and Terminology:
10 - Aligned Unit Materials, Resources and Technology:
11 - Opportunities for Interdisciplinary Connections:
12 - Opportunities for Application of Learning:
13 - Critical Consciousness for Diversity and Equity:
14 - Supporting Multilingual Learners/English Learners (ML/EL):
View all as one page
Next
Relevant Standards:
Major work of the grade is in bold.
The standards that are to be addressed during this unit of study include:
6.EE.B.6Use variables to represent numbers and write expressions when solving a real-world or mathematical problem; understand that a variable can represent an unknown number, or, depending on the purpose at hand, any number in a specified set.
6.EE.B.7Solve real-world and mathematical problems by writing and solving equations of the form x + p = q and px = q for cases in which p, q and x are all nonnegative rational numbers.
6.EE.C.9Use variables to represent two quantities in a real-world problem that change in relationship to one another; write an equation to express one quantity, thought of as the dependent variable, in terms of the other quantity, thought of as the independent variable. Analyze the relationship between the dependent and independent variables using graphs and tables, and relate these to the equation. For example, in a problem involving motion at constant speed, list and graph ordered pairs of distances and times, and write the equation d = 65t to represent the relationship between distance and time.
Examples and Explanations:
6.EE.B.6Connecting writing expressions with story problems and/or drawing pictures will give students a context for this work. It is important for students to read algebraic expressions in a manner that reinforces that the variable represents a number.
Examples:
Maria has three more than twice as many crayons as Elizabeth. Write an algebraic expression to represent the number of crayons that Maria has. (Solution: 2c + 3 where c represents the number of crayons that Elizabeth has.)
An amusement park charges $28 to enter and $0.35 per ticket. Write an algebraic expression to represent the total amount spent. (Solution: 28 + 0.35t where t represents the number of tickets purchased)
Andrew has a summer job doing yard work. He is paid $15 per hour and a $20 bonus when he completes the yard. He was paid $85 for completing one yard. Write an equation to represent the amount of money he earned. (Solution: 15h + 20 = 85 where h is the number of hours worked)
Describe a problem situation that can be solved using the equation 2c + 3 = 15; where c represents the cost of an item.
Bill earned $5.00 mowing the lawn on Saturday. He earned more money on Sunday. Write an expression that shows the amount of money Bill has earned. (Solution: $5.00 + n)
The commutative property can be represented by a + b = b + a where a and b can be any rational number.
6.EE.B.7Students create and solve equations that are based on real world situations. It may be beneficial for students to draw pictures that illustrate the equation in problem situations. Solving equations using reasoning and prior knowledge should be required of students to allow them to develop effective strategies.
Example:
Meagan spent $56.58 on three pairs of jeans. If each pair of jeans costs the same amount, write an algebraic equation that represents this situation and solve to determine how much one pair of jeans cost.
Sample Solution: Students might say: “I created the bar model to show the cost of the three pairs of jeans. Each bar labeled J is the same size because each pair of jeans costs the same amount of money. The bar model represents the equation 3J = $56.58. To solve the problem, I need to divide the total cost of 56.58 between the three pairs of jeans. I know that it will be more than $10 each because 10 x 3 is only 30 but less than $20 each because 20 x 3 is 60. If I start with $15 each, I am up to $45. I have $11.58 left. I then give each pair of jeans $3. That’s $9 more dollars. I only have $2.58 left. I continue until all the money is divided. I ended up giving each pair of jeans another $0.86. Each pair of jeans costs $18.86 (15+3+0.86). I double check that the jeans cost $18.86 each because $18.86 x 3 is $56.58.”
Julio gets paid $20 for babysitting. He spends $1.99 on a package of trading cards and $6.50 on lunch. Write and solve an equation to show how much money Julio has left.(Solution: 20 = 1.99 + 6.50 +x,x= $11.51)
6.EE.C.9 Students can use many forms to represent relationships between quantities. Multiple representations include describing the relationship using language, a table, an equation, or a graph. Translating between multiple representations helps students understand that each form represents the same relationship and provides a different perspective on the function.
Examples:
What is the relationship between the two variables? Write an expression that illustrates the relationship.
Use the graph below to describe the change in y as x increases by 1.
Susan started with $1 in her savings. She plans to add $4 per week to her savings. Use an equation, table and graph to demonstrate the relationship between the number of weeks that pass and the amount in her savings account.
Language: Susan has $1 in her savings account. She is going to save $4 each week.
Equation: y = 4x + 1
Table:
Graph:
Transfer Goal: Aligned to district portrait or vision of the learner
In this unit students will develop the skills of perseverance, reasoning, modeling, and precision. This will be accomplished through focus on the following Standards for Mathematical Practice:
Make sense of problems and persevere in solving them.
Reason abstractly and quantitatively.
Construct viable arguments and critique the reasoning of others
Model with mathematics.
Look for and make use of structure
Grade level content is in bold
Coherence:
How does this unit build on and connect to prior knowledge and learning?
Students build on their previous understandings of:
Using equivalent fractions to add and subtract;
Multiplication and division including multiplication and division of fractions;
Analyzing patterns and relationships;
Arithmetic to apply to algebraic expressions; and
Multiplication and division to divide fractions by fractions.
How does this unit prepare students for future learning?
The learning of this unit serves as a foundation for content that will be addressed in future years. Specifically, students will utilize this learning to:
Solve problems using numerical and algebraic expressions and equations; and
Understand solving equations as a process of reasoning and explain the reasoning
Essential Questions:
Essential Questions can be approached in multiple ways. There should be no more than 2-3 essential questions and they should align with your topics. Questions can be repeated throughout a course or over years, with different enduring understandings.
What is equivalence?
How can properties of operations be used to prove equivalence?
How are variables defined and used?
Enduring Understanding:
The major ideas you want students to internalize and understand deeply. These understandings should be thematic in nature. They are not the end all, be all of the question. They are focused to align to the focus (unit overview).
Students understand:
properties of operations are used to determine if expressions are equivalent;
there is a designated sequence to perform operations (Order of Operations);
variables can be used as unique unknown values or as quantities that vary; and
algebraic expressions may be used to represent and generate mathematical problems and real life situations.
What Students Will Know:
Quantities can be represented in real world problems by variables that change in relationship to each other
Variables can be used to represent, write, and solve equations and inequalities for real world problems
What Students Will Do:
Use variables to represent numbers and write expressions to solve real-world problems
Solve real-world problems using equations with variables where variables are nonnegative rational numbers
Demonstration of Learning:
Smarter Balanced Connections:
Expressions and Equations Interim Block
One Variable Expressions and Equations Focused Block
Dependent and Independent Variables Focused Block
Additional Assessment Samples:
Smarter Balanced Sample Assessment Item 6.EE.7
NWEA Assessment Item 6.EE.9
Unit Specific Vocabulary and Terminology:
The purpose of vocabulary work should be to allow all students to access mathematics. Vocabulary is a way to provide opportunities for students to use mathematical language to communicate about how they solved a problem, describe their reasoning, and demonstrate understanding of mathematical content. Vocabulary is inclusive of key words and phrases.
Often multilingual learners/English learners (MLs/ELs) are perceived as lacking academic language and needing remediation. Research shows that MLs/ELs bring standards-aligned background knowledge and experiences to the task of learning, and they need opportunities to extend their language for academic purposes. When considering the language demand of a lesson (at the word level), you can check for cognates and polysemous words. Pointing out these words to students can help them activate and build background knowledge assumed in lessons. TESOL professionals can assist with the identification of cognates and polysemous words, and they can provide guidance about the background knowledge MLs/ELs bring or may need.
The words with an are words that appear in the Smarter Balanced Construct Relevant Vocabulary for Mathematics intended to ensure that teachers remember to embed these terms in their instruction.
Academic Vocabulary
Solution
Substitution
Variable/unknown
Content Vocabulary
Dependent Variable
Graph
Equation
Independent Variable
Inverse Operation
Solution
Solution Set
Table of Values
X-axis
Y-axis
Relation
Vocabulary resources:
Bilingual Glossaries and Cognates
Using Cognates to Develop Comprehension in English
Challenges for EL Students to Overcome
Cognates and Polysemous Words
Granite School Vocabulary Cards:Each card has the word and a picture. They are designed to help all students with math content vocabulary,including ELL, Gifted and Talented, Special Education, and Regular Education students.
English Math Vocabulary Cards
Spanish Math Vocabulary Cards
Chinese Math Vocabulary Cards
French Math Vocabulary Cards
Aligned Unit Materials, Resources and Technology:
High-quality instructional resources are critical for improving student outcomes. The alignment guidance is intended to clarify content and support understanding for clear implementation and coherence.
Materials selection is a local control decision and these documents have been provided from participating publishers to assist districts in implementation.Use of the materials from these publishers is not required. These aligned core programs meet expectations as reported by edReports. Strong alignment of curricula and instructional materials have the potential to support student engagement and teacher growth.
EdGems Math Grade 6
enVisions Grade 6
Eureka Math Grade 6
HMH Into Math Grade 6
Imagine Learning Illustrative Mathematics Grade 6
i-Ready Math Grade 6
MidSchoolMath Grade 6
Open Up Resouces Math Grade 6
Opportunities for Interdisciplinary Connections:
Science
MS-LS2-3Develop a model to describe the cycling of matter and flow of energy among living and nonliving parts of an ecosystem
MS-LS2-4Construct an argument supported by empirical evidence that changes to physical or biological components of an ecosystem affect populations
MS-LS2-5Evaluate competing design solutions for maintaining biodiversity and ecosystem services
MS-ESS2-6Develop and use a model to describe how unequal heating and rotation of the Earth cause patterns of atmospheric and oceanic circulation that determine regional climates
MS-PS3-1Construct and interpret graphical displays of data to describe the relationships of kinetic energy to the mass of an object and to the speed of an object
MS-LS1-1Conduct an investigation to provide evidence that living things are made of cells; either one cell or many different numbers and types of cells
MS-LS1-2Develop and use models to describe the parts, functions, and basic processes of cells
MS-LS1-3Use argument supported by evidence for how the body is a system of interacting subsystems composed of groups of cells
MS-LS1-6Construct a scientific explanation based on evidence for the role of photosynthesis in the cycling of matter and flow of energy into and out of organisms
MS-LS1-7Develop a model to describe how food molecules (sugar) are rearranged through chemical and/or release energy as this matter moves through an organism
Computer Science
2-AP-11Create clearly named variables that represent different data types and perform operations on their values
ISTE
1cEmpowered Learner
Opportunities for Application of Learning:
Defined Learningprovides an open access online library of standards-aligned project-based lessons to help students meet the expectations of the Standards. Each project is based on a situation in a relevant career to help students connect classroom content to career pathways. This supplemental resource is available at no cost to teachers and districts.Create an account and log in to access this free resource to support your curriculum.
Paramedic
Artificial Island Real Estate
Food Truck Entrepreneur
The tasks below provide additional opportunities to apply the content of this unit.
Firefighter Allocation
Morning Walk
Fruit Salad
Chocolate Bar Sales
Critical Consciousness for Diversity and Equity:
Culturally relevant mathematics engages and empowers students. Opportunities for teachers to orchestrate discussions where students share not only connections to prior mathematics learned but also to their lived experiences must be provided. It is important to dig deep to find ways to link students’ home cultures and the mathematics classroom. Build authentic relationships with families through two-way, reciprocal conversations that acknowledge families’ cultures as assets for teaching and learning. As you plan to implement this unit, focus on designing experiences that have students at the center. In addition to keeping students engaged, ensure the learning experiences have a context that reflects lived experiences (mirror) or provide opportunities to view and learn about the broader world (window).
One crucial link to students’ home cultures is through their language. Students’ language repertoires –all the languages and language varieties they use everyday– are a valuable resource to be engaged in the mathematics classroom. This approach is referred to as a translanguaging stance. It is based on a dynamic view of bilingualism that understands individuals as having one linguistic repertoire composed of various named languages (such as English and Spanish) and/or language varieties on which they draw to make meaning.
The following questions are intended to assist in promoting diverse voices and perspectives while avoiding bias and stereotyping:
How will students share their experiences with others while attending to the mathematics in the unit?
What opportunities are there for students to make connections from their life to the mathematics?
What do I know or need to learn about my students to create lessons free from bias and stereotypes?
In what ways can the mathematical thinking already taking place in the classroom and community be honored?
How is relevant background knowledge developed so that all students can access the mathematics of the unit?
What opportunities are there for students to use their full language repertoires during mathematical discussions and practice? Where can I create these opportunities?
What do I know or need to learn about students’ languages and how they use them? How can I learn this?
Visit the Culturally Responsive Teaching Collection for additional resources
Supporting Multilingual Learners/English Learners (ML/EL):
Mathematical symbols, expressions, and methods are not universal; ways of doing math differ across cultures. When working with diverse students, especially with those from different countries, it is important to be aware that these differences exist.
It is also important to remember that communicating about mathematical content and practices requires complex language. Since conceptual learning and language learning are interconnected and acquired through participation in meaningful activities, the research-based strategies listed below focus on making content comprehensible (accessible) and creating opportunities for student voice, both verbal and written.
Additional resources for ML/EL
CELP Standards--Linguistic Supports
ML/EL Support Collection for Math
This unit presents opportunity to address the following CELP Standards:
CELP Standard 1:Construct meaning from oral presentations and literary and informational text through grade-appropriate listening, reading, and viewing
CELP Standard 2:Participate in grade-appropriate oral and written exchanges of information, ideas, and analyses, responding to peer, audience, or reader comments and questions
CELP Standard 3:Speak and write about grade-appropriate complex literary and informational texts and topics
CELP Standard 4:Construct grade-appropriate oral and written claims and support them with
reasoning and evidence
CELP Standard 5:Conduct research and evaluate and communicate findings to answer questions or solve problems
CELP Standard 6:Analyze and critique the arguments of others orally and in writing
CELP Standard 7:Adapt language choices to purpose, task, and audience when speaking and writing
CELP Standard 8:Determine the meaning of words and phrases in oral presentations and literary and informational text
CELP Standard 9:Create clear and coherent grade-appropriate speech and text
The document below provides guidance on these standards that is grade appropriate and broken down by language level descriptors which will assist the teacher in making the content of the unit accessible to all students.
Grade 6 Language Level Descriptors
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Title
1 - Relevant Standards:
2 - Examples and Explanations:
3 - Transfer Goal: Aligned to district portrait or vision of the learner
4 - Essential Questions:
5 - Enduring Understanding:
6 - What Students Will Know:
7 - What Students Will Do:
8 - Demonstration of Learning:
9 - Unit Specific Vocabulary and Terminology:
10 - Aligned Unit Materials, Resources and Technology:
11 - Opportunities for Interdisciplinary Connections:
12 - Opportunities for Application of Learning:
13 - Critical Consciousness for Diversity and Equity:
14 - Supporting Multilingual Learners/English Learners (ML/EL):
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11361 | https://precalculuscoach.com/wp-content/uploads/2017/10/5-2-Assignment-Verifying-Trigonometric-Identities.pdf | Name: _______ Period: __ Date: ___ Verifying Trigonometric Identities Assignment Copyright ©PreCalculusCoach.com 1 Verify each identity. 1. 𝒔𝒆𝒄𝟐𝜽(𝟏−𝒄𝒐𝒔𝟐𝜽) = 𝒕𝒂𝒏𝟐𝜽 2. 𝒕𝒂𝒏𝜽𝒄𝒐𝒔𝒆𝒄𝟐𝜽−𝒕𝒂𝒏𝜽= 𝒄𝒐𝒕𝜽 3. 𝒔𝒆𝒄𝜽 𝒔𝒊𝒏𝜽− 𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝜽= 𝒄𝒐𝒕𝜽 4. 𝒄𝒐𝒔𝜽−𝒄𝒐𝒔𝜽. 𝒔𝒊𝒏𝟐𝜽= 𝒄𝒐𝒔𝟑𝜽 Name: _______ Period: _ Date: __ Verifying Trigonometric Identities Assignment Copyright ©PreCalculusCoach.com 2 Verify each identity. 1. 𝒔𝒊𝒏𝜽 𝟏−𝒄𝒐𝒔𝜽+ 𝟏−𝒄𝒐𝒔𝜽 𝒔𝒊𝒏𝜽= 𝟐𝒄𝒐𝒔𝒆𝒄𝜽 2. 𝒄𝒐𝒔𝜽 𝟏+𝒔𝒊𝒏𝜽+ 𝒕𝒂𝒏𝜽= 𝒔𝒆𝒄𝜽 Name: _______ Period: __ Date: ___ Verifying Trigonometric Identities Assignment Copyright ©PreCalculusCoach.com 3 3. 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽+𝟏+ 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽−𝟏= 𝟐𝒔𝒆𝒄𝟐𝜽𝒔𝒊𝒏𝜽 4. 𝟏 𝟏−𝒔𝒊𝒏𝜽+ 𝟏 𝟏+𝒔𝒊𝒏𝜽= 𝟐𝒔𝒆𝒄𝟐𝜽 Name: _______ Period: _ Date: __ Verifying Trigonometric Identities Assignment Copyright ©PreCalculusCoach.com 4 Answers Verify each identity. 1. 𝒔𝒆𝒄𝟐𝜽(𝟏−𝒄𝒐𝒔𝟐𝜽) = 𝒕𝒂𝒏𝟐𝜽 Take L.H.S: 𝒔𝒆𝒄𝟐𝜽(𝟏−𝒄𝒐𝒔𝟐𝜽) = 𝒔𝒆𝒄𝟐𝜽−𝒔𝒆𝒄𝟐𝜽𝒄𝒐𝒔𝟐𝜽 = 𝒔𝒆𝒄𝟐𝜽− 𝟏 𝒄𝒐𝒔𝟐𝜽𝒄𝒐𝒔𝟐𝜽 (Reciprocal Identity) = 𝒔𝒆𝒄𝟐𝜽−𝟏 = 𝒕𝒂𝒏𝟐𝜽 (Pythagorean Identity) = R.H.S → 𝒔𝒆𝒄𝟐𝜽(𝟏−𝒄𝒐𝒔𝟐𝜽) = 𝒕𝒂𝒏𝟐𝜽 2. 𝒕𝒂𝒏𝜽𝒄𝒐𝒔𝒆𝒄𝟐𝜽−𝒕𝒂𝒏𝜽= 𝒄𝒐𝒕𝜽 Take L.H.S: 𝒕𝒂𝒏𝜽𝒄𝒐𝒔𝒆𝒄𝟐𝜽−𝒕𝒂𝒏𝜽= 𝒕𝒂𝒏𝜽(𝒄𝒐𝒔𝒆𝒄𝟐𝜽−𝟏) = 𝒕𝒂𝒏𝜽. (𝒄𝒐𝒕𝟐𝜽) (Pythagorean Identity) = 𝒕𝒂𝒏𝜽. ( 𝟏 𝒕𝒂𝒏𝟐𝜽) (Reciprocal Identity) = 𝟏 𝒕𝒂𝒏𝜽= 𝒄𝒐𝒕𝜽 (Reciprocal Identity) = R.H.S → 𝒕𝒂𝒏𝜽𝒄𝒐𝒔𝒆𝒄𝟐𝜽−𝒕𝒂𝒏𝜽= 𝒄𝒐𝒕𝜽 3. 𝒔𝒆𝒄𝜽 𝒔𝒊𝒏𝜽− 𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝜽= 𝒄𝒐𝒕𝜽 Take L.H.S: 𝒔𝒆𝒄𝜽 𝒔𝒊𝒏𝜽− 𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝜽= 𝟏 𝒄𝒐𝒔𝜽 𝒔𝒊𝒏𝜽− 𝒔𝒊𝒏𝟐𝜽 𝒔𝒊𝒏𝜽𝒄𝒐𝒔𝜽 (Reciprocal Identity) = 𝟏 𝒔𝒊𝒏𝜽𝒄𝒐𝒔𝜽− 𝒔𝒊𝒏𝟐𝜽 𝒔𝒊𝒏𝜽𝒄𝒐𝒔𝜽 = 𝟏 − 𝒔𝒊𝒏𝟐𝜽 𝒔𝒊𝒏𝜽𝒄𝒐𝒔𝜽= 𝒄𝒐𝒔𝟐𝜽 𝒔𝒊𝒏𝜽𝒄𝒐𝒔𝜽 (Pythagorean Identity) 𝒄𝒐𝒔𝟐𝜽 𝒔𝒊𝒏𝜽𝒄𝒐𝒔𝜽= 𝒄𝒐𝒔𝜽 𝒔𝒊𝒏𝜽= 𝒄𝒐𝒕𝜽 (Quotient Identity) → 𝒔𝒆𝒄𝜽 𝒔𝒊𝒏𝜽− 𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝜽= 𝒄𝒐𝒕𝜽 4. 𝒄𝒐𝒔𝜽−𝒄𝒐𝒔𝜽. 𝒔𝒊𝒏𝟐𝜽= 𝒄𝒐𝒔𝟑𝜽 Take L.H.S: 𝒄𝒐𝒔𝜽−𝒄𝒐𝒔𝜽. 𝒔𝒊𝒏𝟐𝜽= 𝒄𝒐𝒔𝜽(𝟏−𝒔𝒊𝒏𝟐𝜽) = 𝒄𝒐𝒔𝜽(𝒄𝒐𝒔𝟐𝜽) (Pythagorean Identity) = 𝒄𝒐𝒔𝟑𝜽 = R.H.S → 𝒄𝒐𝒔𝜽−𝒄𝒐𝒔𝜽. 𝒔𝒊𝒏𝟐𝜽= 𝒄𝒐𝒔𝟑𝜽 Name: _______ Period: __ Date: ___ Verifying Trigonometric Identities Assignment Copyright ©PreCalculusCoach.com 5 Verify each identity. 1. 𝒔𝒊𝒏𝜽 𝟏−𝒄𝒐𝒔𝜽+ 𝟏−𝒄𝒐𝒔𝜽 𝒔𝒊𝒏𝜽= 𝟐𝒄𝒐𝒔𝒆𝒄𝜽 Take L.H.S: 𝒔𝒊𝒏𝜽(𝒔𝒊𝒏𝜽)+(𝟏−𝒄𝒐𝒔𝜽)(𝟏−𝒄𝒐𝒔𝜽) (𝟏−𝒄𝒐𝒔𝜽)𝒔𝒊𝒏𝜽 = 𝒔𝒊𝒏𝟐𝜽+(𝟏−𝒄𝒐𝒔𝜽)𝟐 𝒔𝒊𝒏𝜽(𝟏−𝒄𝒐𝒔𝜽) = 𝒔𝒊𝒏𝟐𝜽+𝟏+𝒄𝒐𝒔𝟐𝜽−𝟐𝒄𝒐𝒔𝜽 𝒔𝒊𝒏𝜽(𝟏−𝒄𝒐𝒔𝜽) = 𝟐−𝟐𝒄𝒐𝒔𝜽 𝒔𝒊𝒏𝜽(𝟏−𝒄𝒐𝒔𝜽) (Pythagorean Identity) = 𝟐(𝟏−𝒄𝒐𝒔𝜽) 𝒔𝒊𝒏𝜽(𝟏−𝒄𝒐𝒔𝜽) = 𝟐 𝒔𝒊𝒏𝜽 = 𝟐𝒄𝒐𝒔𝒆𝒄𝜽= R.H.S (Reciprocal Identity) → 𝒔𝒊𝒏𝜽 𝟏−𝒄𝒐𝒔𝜽+ 𝟏−𝒄𝒐𝒔𝜽 𝒔𝒊𝒏𝜽= 𝟐𝒄𝒐𝒔𝒆𝒄𝜽 2. 𝒄𝒐𝒔𝜽 𝟏+𝒔𝒊𝒏𝜽+ 𝒕𝒂𝒏𝜽= 𝒔𝒆𝒄𝜽 Take L.H.S: 𝒄𝒐𝒔𝜽 𝟏+𝒔𝒊𝒏𝜽+ 𝒕𝒂𝒏𝜽= 𝒄𝒐𝒔𝜽+(𝟏+𝒔𝒊𝒏𝜽)𝒕𝒂𝒏𝜽 𝟏+𝒔𝒊𝒏𝜽 = 𝒄𝒐𝒔𝜽+(𝟏+𝒔𝒊𝒏𝜽)𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝜽 𝟏+𝒔𝒊𝒏𝜽 (Reciprocal Identity) = 𝒄𝒐𝒔𝜽+𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝜽+𝒔𝒊𝒏𝟐𝜽 𝒄𝒐𝒔𝜽 (𝟏+𝒔𝒊𝒏𝜽) = 𝒄𝒐𝒔𝟐𝜽+ 𝒔𝒊𝒏𝜽+𝒔𝒊𝒏𝟐𝜽 𝒄𝒐𝒔𝜽 (𝟏+𝒔𝒊𝒏𝜽) = 𝟏+ 𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝜽(𝟏+𝒔𝒊𝒏𝜽) (Pythagorean Identity) = 𝟏 𝒄𝒐𝒔𝜽= 𝒔𝒆𝒄𝜽= R.H.S (Reciprocal Identity) → 𝒄𝒐𝒔𝜽 𝟏+𝒔𝒊𝒏𝜽+ 𝒕𝒂𝒏𝜽= 𝒔𝒆𝒄𝜽 Name: _______ Period: _ Date: __ Verifying Trigonometric Identities Assignment Copyright ©PreCalculusCoach.com 6 3. 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽+𝟏+ 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽−𝟏= 𝟐𝒔𝒆𝒄𝟐𝜽𝒔𝒊𝒏𝜽 Take L.H.S: 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽+𝟏+ 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽−𝟏= 𝒄𝒐𝒔𝒆𝒄𝜽−𝟏+𝒄𝒐𝒔𝒆𝒄𝜽+𝟏 (𝒄𝒐𝒔𝒆𝒄𝜽+𝟏)(𝒄𝒐𝒔𝒆𝒄𝜽−𝟏) = 𝟐𝒄𝒐𝒔𝒆𝒄𝜽 𝒄𝒐𝒔𝒆𝒄𝟐𝜽−𝟏 = 𝟐𝒄𝒐𝒔𝒆𝒄𝜽 𝒄𝒐𝒕𝟐𝜽 (Pythagorean Identity) = 𝟐 𝒔𝒊𝒏𝜽× 𝒔𝒊𝒏𝟐𝜽 𝒄𝒐𝒔𝟐𝜽 (Pythagorean Identity) = 𝟐𝒔𝒊𝒏𝜽 𝒄𝒐𝒔𝟐𝜽= 𝟐𝒔𝒆𝒄𝟐𝜽𝒔𝒊𝒏𝜽= R.H.S (Reciprocal Identity) → 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽+𝟏+ 𝟏 𝒄𝒐𝒔𝒆𝒄𝜽−𝟏= 𝟐𝒔𝒆𝒄𝟐𝜽𝒔𝒊𝒏𝜽 4. 𝟏 𝟏−𝒔𝒊𝒏𝜽+ 𝟏 𝟏+𝒔𝒊𝒏𝜽= 𝟐𝒔𝒆𝒄𝟐𝜽 Take L.H.S: 𝟏 𝟏−𝒔𝒊𝒏𝜽+ 𝟏 𝟏+𝒔𝒊𝒏𝜽= 𝟏+𝒔𝒊𝒏𝜽+𝟏−𝒔𝒊𝒏𝜽 (𝟏−𝒔𝒊𝒏𝜽)(𝟏+𝒔𝒊𝒏𝜽) = 𝟐 𝟏−𝒔𝒊𝒏𝟐𝜽 = 𝟐 𝒄𝒐𝒔𝟐𝜽 (Pythagorean Identity) = 𝟐𝒔𝒆𝒄𝟐𝜽= R.H.S (Reciprocal Identity) → 𝟏 𝟏−𝒔𝒊𝒏𝜽+ 𝟏 𝟏+𝒔𝒊𝒏𝜽= 𝟐𝒔𝒆𝒄𝟐𝜽 |
11362 | https://www.passporthealthusa.com/2019/04/dr-john-snow-and-the-origin-of-epidemiology/ | Dr. John Snow and the Origin of Epidemiology
April 5, 2019 by Will Sowards 1 Comment
Today, epidemiology is a valuable field of study which plays a role in eradicating diseases. It helps us prevent outbreaks, craft preventative measures and treat illnesses.
But, it wasn’t so long ago that the world didn’t have this practice and suffered much more drastic consequences from each case of sickness.
Stories of the most rudimentary vaccines stretch back a few hundred years, but epidemiology is a bit younger.
Described by Merriam Webster as, “medical science that deals with the incidence, distribution, and control of disease in a population,” epidemiology’s origins are largely credited to legendary Victorian doctor John Snow. His claim to fame in discovering that cholera is spread by a parasite through contaminated water or food. Snow’s work even earned the nickname “the father of epidemiology.”
Image courtesy of Rsabbatini on English Wikipedia.
John Snow: The Father of Epidemiology
Snow’s cholera discovery began in late 1848, when a deadly outbreak of Asian cholera struck London.
Though it wasn’t unlike ones before it, it acted as an epidemiological testing ground for John Snow. He used the outbreak to challenge the community belief that cholera was an airborne disease.
At the time the prevailing “miasma” theory was that cholera was spread by rising poisonous gases and decaying particles. But, John Snow was highly skeptical of this theory.
In the past, Snow had treated sick coal-miners who caught cholera while working deep underground raised. Instead Snow surmised that the disease may have been spread through invisible germs. With no ability to wash their hands while working, this would make for an easy opportunity to spread bacteria.
So, when the 1848 outbreak began, Snow took the opportunity to undertake a thorough investigation.
To begin his research, Snow started with the first victim. He learned all he could about the circumstances surrounding the merchant seaman who died a short time after renting a room in London. Snow questioned the landlord and the attending physician to follow the path of the disease. He learned that the next tenant in the room had also contracted cholera and died.
The path of cholera showed that left-behind germs could be the culprit.
Next, through countless interviews, Snow found that victims all first reported digestive issues. Problems such as diarrhea would indicate that the disease was spread through food or water rather than the air. At the time, Snow knew that food and water-borne disease would often show with symptoms in the stomach. Airborne diseases would instead first cause respiratory symptoms.
This piece of information, and others like it, taught Snow that cholera epidemics were seemingly brought on by poor sanitary conditions. Poor separation of water sources would easily contaminate wells and water pipes. With waste from sewers and drains in the mix, a water-borne disease could move travel.
John Snow Shares His Findings
The next year he compiled his findings and released a 39-page essay entitled “On the Mode of Communication of Cholera”. The pamphlet was paid for out of Snow’s own pocket and fully explored the research he had done into cholera.
At the time, it was not received well by many, such as The Lancet founding editor Thomas Wakley. Wakley came down particularly harshly on Snow, publishing his criticism. “In riding his hobby very hard, he has fallen down through a gully-hole and has never since been able to get out again.”
Snow wasn’t deterred.
When cholera broke out in the district Snow was working in the following summer, he immediately worked on his water theory. He sorted through municipal records for the source of this outbreak.
He found that two private companies supplied the water used in the district. UCLA shares that one company, the Southwark and Vauxhall Water Company, sourced its water from a sewage-polluted Thames area. The other company, the Lambeth Water Company, had recently moved its intake facilities above sewer outlets.
It was this moment when his grand experiment began.
Snow conducted survey after survey to find out which houses had water from which company. Eventually he realized that in one four-week period a staggering 286 of the 334 cholera victims got water from the Southwark and Vauxhall Water Company. During that period, just 14 victims received water from the Lambeth Water Company.
He would then write of the dire conditions putting a whole region in danger.
“No fewer than three hundred thousand people of both sexes, of every age and occupation, and of every rank and station, from gentle folks down to the very poor, were divided into two groups without their choice, and, in most cases, without their knowledge; one group being supplied with water containing the sewage of London, and amongst it, whatever might have come from the cholera patients-the other group having water quite free from such impurity.”
Again, his peers were not persuaded.
Another Outbreak Gives Dr. Snow More Proof
Snow needed to wait until 1854 for another breakthrough. It was in this year that the Broad Street cholera outbreak offered another opportunity.
Within a week of the outbreak’s beginning, people fled their homes. Dead victims were being taken away by the cartload. Most of the fatalities occurred in the vicinity of a pump on Broad Street. Snow suspected that although the companies that supplied water to Broad Street were generally reliable, the well under the pump might have been contaminated by nearby sewage pipes.
When sampling the water proved unhelpful, Snow plotted a large map with victim information.
He found that 73 of the 83 deaths happened in homes close to the Broad Street pump. Then, after interviewing those at the homes of the other victims, Snow found that eight of 10 victims drank the pump water. With final research, he concluded that 61 of the 83 victims had drunk water from the Broad Street pump.
In a meeting with the Board of Guardians, Snow presented his findings. He recommended the Board remove the Broad Street pump handle immediately. This way, no more people would be able to drink the water and get infected.
The listeners were highly skeptical but agreed, and the local outbreak shortly ended.
The Father of Epidemiology and His Legacy
Despite this link, Snow’s theory regarding cholera still was not accepted by many of his peers. It was until a decade after his death in 1858 that evidence was found to prove his cholera theories.
In his lifetime John Snow was considered ridiculous by many for his epidemiological views on cholera. He was instead famous as an anesthetist, deemed the most accomplished in the British Isles.
Much of this reputation was likely garnered from his assistance to Queen Victoria during the births of two of her children, Prince Leopold and Princess Beatrice. In fact, many readers today may be familiar with John Snow due to his recent feature on the PBS Masterpiece showing of Victoria.
In the end, Snow was a medical genius who pioneered multiple techniques in both epidemiology and anesthesiology. Upon hearing the name John Snow, many of us likely imagine the one who grew up in Winterfell. But, it’s clear that the phrase “You know nothing Jon Snow” wouldn’t apply to the Father of Epidemiology.
Had you heard of Dr. John Snow before this article? Did you know the field of epidemiology had such relatively recent roots? Let us know in the comments below, or via Facebook and Twitter.
Written for Passport Health by Katherine Meikle. Katherine is a research writer and proud first-generation British-American living in Florida, where she was born and raised. She has a passion for travel and a love of writing, which go hand-in-hand.
Filed Under: General Posts
Comments
Chris says
Chris says
April 21, 2020 at 7:59 pm
Katherine, very well written article about Dr. John Snow, and yes last year I became familiar with Dr. Snow’s landmark use of geospatial Epidemiology only because I was watching “Victoria”on Masterpiece Theatre. It is right on point today with understanding the current Covid19 Pandemic, but unfortunately I’ve come to the belief that many Americans, especially our media journalists and commentators, are lacking a historical understanding of the basis of mapping out disease.
I was wondering if you are familiar with the recent findings from classified WW1 records that the 1918 Pandemic also had its origins traced to China; and that influenza got out of China due to the importation of Infected Chinese laborers to the UK and France during WW1 due to manpower shortages that developed. I ran across that information recently from a google search on the 1918 Influenza Pandemic and whether there was any connection to China.
Good luck on future writing. Cpw
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Former Santa Cruz County treasurer sentenced to 10 years in prison for stealing over $38 million in county funds
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Date:June 24, 2025
Contact:newsroom@ci.irs.gov
Tucson, AZ — Elizabeth Gutfahr, of Rio Rico, Arizona, was sentenced on June 23, 2025, by United States District Judge Rosemary C. Márquez to 120 months in prison, followed by three years of supervised release. Gutfahr previously pleaded guilty to Embezzlement by a Public Official, Money Laundering, and Tax Evasion. Gutfahr was also ordered to pay approximately $51.8 million in restitution to Santa Cruz County and the United States Treasury.
“The people of Santa Cruz County and all Arizonans have a right to expect their elected leaders to serve with integrity and in the best interest of their constituents,” said U.S. Attorney Timothy Courchaine. “Ms. Gutfahr stole more than money from the people of her county, she betrayed the confidence of the voters who elected her. This sentence shows that abuse of public trust will be punished.”
“Ms. Gutfahr violated her sworn duty by enriching herself with the public money she was entrusted to protect,” said Special Agent in Charge Carissa Messick of the IRS Criminal Investigation Phoenix Field Office. “Taxpayers deserve to know that their elected leaders are working in the community’s best interest — not just their own. IRS-CI remains committed to rooting out corruption at every level.”
“Ms. Gutfahr will now be held accountable for using her official position for huge financial gain at the expense of the residents of Santa Cruz County,” said FBI Phoenix Special Agent in Charge Heith Janke. “Each act of greed and dishonor negatively affected fundamental aspects of the county’s operations. The FBI continues to investigate public corruption cases, and we remain committed to identifying and pursuing those who violate the public’s trust.”
According to court documents, Gutfahr, who served as Santa Cruz County Treasurer from 2012 through 2024, embezzled and laundered approximately $38.7 million by wiring public funds from Santa Cruz County’s account to accounts in the names of fake companies she had created that performed no legitimate business. Gutfahr then used the money to purchase real estate, to renovate her family ranch, to pay expenses for her cattle business, and to buy at least 20 vehicles.
Gutfahr’s 10-year scheme involved approximately 187 wire transfers, which she was able to complete by undermining the two-step approval process required for transfers. Gutfahr used the token of a subordinate Santa Cruz County employee so that she could both initiate and approve the wire transfers. To cover up the scheme, Gutfahr falsified accounting records, cash reconciliation records, and reports of the County’s investment accounts, thereby hiding the millions of dollars that she had stolen from Santa Cruz County. Gutfahr also failed to report any of the stolen funds as income for tax purposes.
IRS-CI and the FBI conducted the investigation in this case. Assistant U.S. Attorney Jane L. Westby for the District of Arizona and Senior Litigation Counsel Nicholas W. Cannon of the Criminal Division’s Public Integrity Section handled the prosecution.
IRS Criminal Investigation (IRS-CI) is the law enforcement arm of the IRS, responsible for conducting financial crime investigations, including tax fraud, narcotics trafficking, money laundering, public corruption, healthcare fraud, identity theft and more. IRS-CI special agents are the only federal law enforcement agents with investigative jurisdiction over violations of the Internal Revenue Code, obtaining a 90% federal conviction rate. The agency has 19 field offices located across the U.S. and 14 attaché posts abroad.
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11364 | https://math.stackexchange.com/questions/303939/planar-graph-number-of-faces | Skip to main content
Planar graph, number of faces
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I need to determine the number of faces of a planar graph with n vertices, m edges and k connected components. I was thinking of using Euler's formula f=m−n+2 but that is for a connected graph. Because I have k components I was thinking k times Euler formula, for each connected component.
Any advice or help is welcome.
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My advice would be to draw a bunch of examples with, say, three connected components, and calculate f−m+n for each of them, and make a conjecture, and prove it. If you get stuck along the way, come back, tell us what you've done, and someone will help.
– Gerry Myerson
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In the Euler's formula for a connected planar graph f−m+n=2, one of the face is the exterior face. If you only count the inner face, it is finner−m+n=1. If you have k connected component, you get finner−m+n=k. Add back the exterior face, you get f−m+n=k+1.
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We will count the outer face as its own face. So a cycle has two faces, for example.
The idea is to take each connected component C1, C2, etc., and connect them by drawing a bridge between C1 and C2, C2 and C3, etc. We will thus add n−1 edges (the restriction is if you contract the connected components we had previously, you must form a tree).
F=f remains the same.
V=n since no vertices were added.
E=m+k−1 since k−1 edges were added.
Now apply Euler's formula.
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Euler's formula can be extended
V+F=E+C+χ,
where C is the number of components and χ is Euler's characteristic of the surface where the graph lives on. If you deal with k-regular planar graphs the mean face degree obeys:
∑fkF=2kk−2(1−1+χF)
(see here)
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11365 | https://www.mathway.com/popular-problems/Calculus/545604 | Evaluate the Limit limit as t approaches 0 of (te^t)/(1-e^t) | Mathway
Enter a problem...
[x]
Calculus Examples
Popular Problems
Calculus
Evaluate the Limit limit as t approaches 0 of (te^t)/(1-e^t)
lim t→0 t e t 1−e t lim t→0t e t 1-e t
Step 1
Apply L'Hospital's rule.
Tap for more steps...
Step 1.1
Evaluate the limit of the numerator and the limit of the denominator.
Tap for more steps...
Step 1.1.1
Take the limit of the numerator and the limit of the denominator.
lim t→0 t e t lim t→0 1−e t lim t→0t e t lim t→01-e t
Step 1.1.2
Evaluate the limit of the numerator.
Tap for more steps...
Step 1.1.2.1
Split the limit using the Product of Limits Rule on the limit as t t approaches 0 0.
lim t→0 t⋅lim t→0 e t lim t→0 1−e t lim t→0t⋅lim t→0e t lim t→01-e t
Step 1.1.2.2
Move the limit into the exponent.
lim t→0 t⋅e lim t→0 t lim t→0 1−e t lim t→0t⋅e lim t→0t lim t→01-e t
Step 1.1.2.3
Evaluate the limits by plugging in 0 0 for all occurrences of t t.
Tap for more steps...
Step 1.1.2.3.1
Evaluate the limit of t t by plugging in 0 0 for t t.
0⋅e lim t→0 t lim t→0 1−e t 0⋅e lim t→0t lim t→01-e t
Step 1.1.2.3.2
Evaluate the limit of t t by plugging in 0 0 for t t.
0⋅e 0 lim t→0 1−e t 0⋅e 0 lim t→01-e t
0⋅e 0 lim t→0 1−e t 0⋅e 0 lim t→01-e t
Step 1.1.2.4
Simplify the answer.
Tap for more steps...
Step 1.1.2.4.1
Anything raised to 0 0 is 1 1.
0⋅1 lim t→0 1−e t 0⋅1 lim t→01-e t
Step 1.1.2.4.2
Multiply 0 0 by 1 1.
0 lim t→0 1−e t 0 lim t→01-e t
0 lim t→0 1−e t 0 lim t→01-e t
0 lim t→0 1−e t 0 lim t→01-e t
Step 1.1.3
Evaluate the limit of the denominator.
Tap for more steps...
Step 1.1.3.1
Evaluate the limit.
Tap for more steps...
Step 1.1.3.1.1
Split the limit using the Sum of Limits Rule on the limit as t t approaches 0 0.
0 lim t→0 1−lim t→0 e t 0 lim t→01-lim t→0e t
Step 1.1.3.1.2
Evaluate the limit of 1 1 which is constant as t t approaches 0 0.
0 1−lim t→0 e t 0 1-lim t→0e t
Step 1.1.3.1.3
Move the limit into the exponent.
0 1−e lim t→0 t 0 1-e lim t→0t
0 1−e lim t→0 t 0 1-e lim t→0t
Step 1.1.3.2
Evaluate the limit of t t by plugging in 0 0 for t t.
0 1−e 0 0 1-e 0
Step 1.1.3.3
Simplify the answer.
Tap for more steps...
Step 1.1.3.3.1
Simplify each term.
Tap for more steps...
Step 1.1.3.3.1.1
Anything raised to 0 0 is 1 1.
0 1−1⋅1 0 1-1⋅1
Step 1.1.3.3.1.2
Multiply−1-1 by 1 1.
0 1−1 0 1-1
0 1−1 0 1-1
Step 1.1.3.3.2
Subtract 1 1 from 1 1.
0 0 0 0
Step 1.1.3.3.3
The expression contains a division by 0 0. The expression is undefined.
Undefined
0 0 0 0
Step 1.1.3.4
The expression contains a division by 0 0. The expression is undefined.
Undefined
0 0 0 0
Step 1.1.4
The expression contains a division by 0 0. The expression is undefined.
Undefined
0 0 0 0
Step 1.2
Since 0 0 0 0 is of indeterminate form, apply L'Hospital's Rule. L'Hospital's Rule states that the limit of a quotient of functions is equal to the limit of the quotient of their derivatives.
lim t→0 t e t 1−e t=lim t→0 d d t[t e t]d d t[1−e t]lim t→0t e t 1-e t=lim t→0d d t[t e t]d d t[1-e t]
Step 1.3
Find the derivative of the numerator and denominator.
Tap for more steps...
Step 1.3.1
Differentiate the numerator and denominator.
lim t→0 d d t[t e t]d d t[1−e t]lim t→0d d t[t e t]d d t[1-e t]
Step 1.3.2
Differentiate using the Product Rule which states that d d t[f(t)g(t)]d d t[f(t)g(t)] is f(t)d d t[g(t)]+g(t)d d t[f(t)]f(t)d d t[g(t)]+g(t)d d t[f(t)] where f(t)=t f(t)=t and g(t)=e t g(t)=e t.
lim t→0 t d d t[e t]+e t d d t[t]d d t[1−e t]lim t→0t d d t[e t]+e t d d t[t]d d t[1-e t]
Step 1.3.3
Differentiate using the Exponential Rule which states that d d t[a t]d d t[a t] is a t ln(a)a t ln(a) where a a=e e.
lim t→0 t e t+e t d d t[t]d d t[1−e t]lim t→0t e t+e t d d t[t]d d t[1-e t]
Step 1.3.4
Differentiate using the Power Rule which states that d d t[t n]d d t[t n] is n t n−1 n t n-1 where n=1 n=1.
lim t→0 t e t+e t⋅1 d d t[1−e t]lim t→0t e t+e t⋅1 d d t[1-e t]
Step 1.3.5
Multiply e t e t by 1 1.
lim t→0 t e t+e t d d t[1−e t]lim t→0t e t+e t d d t[1-e t]
Step 1.3.6
By the Sum Rule, the derivative of 1−e t 1-e t with respect to t t is d d t+d d t[−e t]d d t+d d t[-e t].
lim t→0 t e t+e t d d t+d d t[−e t]lim t→0t e t+e t d d t+d d t[-e t]
Step 1.3.7
Since 1 1 is constant with respect to t t, the derivative of 1 1 with respect to t t is 0 0.
lim t→0 t e t+e t 0+d d t[−e t]lim t→0t e t+e t 0+d d t[-e t]
Step 1.3.8
Evaluate d d t[−e t]d d t[-e t].
Tap for more steps...
Step 1.3.8.1
Since −1-1 is constant with respect to t t, the derivative of −e t-e t with respect to t t is −d d t[e t]-d d t[e t].
lim t→0 t e t+e t 0−d d t[e t]lim t→0t e t+e t 0-d d t[e t]
Step 1.3.8.2
Differentiate using the Exponential Rule which states that d d t[a t]d d t[a t] is a t ln(a)a t ln(a) where a a=e e.
lim t→0 t e t+e t 0−e t lim t→0t e t+e t 0-e t
lim t→0 t e t+e t 0−e t lim t→0t e t+e t 0-e t
Step 1.3.9
Subtract e t e t from 0 0.
lim t→0 t e t+e t−e t lim t→0t e t+e t-e t
lim t→0 t e t+e t−e t lim t→0t e t+e t-e t
lim t→0 t e t+e t−e t lim t→0t e t+e t-e t
Step 2
Evaluate the limit.
Tap for more steps...
Step 2.1
Split the limit using the Limits Quotient Rule on the limit as t t approaches 0 0.
lim t→0 t e t+e t lim t→0−e t lim t→0t e t+e t lim t→0-e t
Step 2.2
Split the limit using the Sum of Limits Rule on the limit as t t approaches 0 0.
lim t→0 t e t+lim t→0 e t lim t→0−e t lim t→0t e t+lim t→0e t lim t→0-e t
Step 2.3
Split the limit using the Product of Limits Rule on the limit as t t approaches 0 0.
lim t→0 t⋅lim t→0 e t+lim t→0 e t lim t→0−e t lim t→0t⋅lim t→0e t+lim t→0e t lim t→0-e t
Step 2.4
Move the limit into the exponent.
lim t→0 t⋅e lim t→0 t+lim t→0 e t lim t→0−e t lim t→0t⋅e lim t→0t+lim t→0e t lim t→0-e t
Step 2.5
Move the limit into the exponent.
lim t→0 t⋅e lim t→0 t+e lim t→0 t lim t→0−e t lim t→0t⋅e lim t→0t+e lim t→0t lim t→0-e t
Step 2.6
Move the term−1-1 outside of the limit because it is constant with respect to t t.
lim t→0 t⋅e lim t→0 t+e lim t→0 t−lim t→0 e t lim t→0t⋅e lim t→0t+e lim t→0t-lim t→0e t
Step 2.7
Move the limit into the exponent.
lim t→0 t⋅e lim t→0 t+e lim t→0 t−e lim t→0 t lim t→0t⋅e lim t→0t+e lim t→0t-e lim t→0t
lim t→0 t⋅e lim t→0 t+e lim t→0 t−e lim t→0 t lim t→0t⋅e lim t→0t+e lim t→0t-e lim t→0t
Step 3
Evaluate the limits by plugging in 0 0 for all occurrences of t t.
Tap for more steps...
Step 3.1
Evaluate the limit of t t by plugging in 0 0 for t t.
0⋅e lim t→0 t+e lim t→0 t−e lim t→0 t 0⋅e lim t→0t+e lim t→0t-e lim t→0t
Step 3.2
Evaluate the limit of t t by plugging in 0 0 for t t.
0⋅e 0+e lim t→0 t−e lim t→0 t 0⋅e 0+e lim t→0t-e lim t→0t
Step 3.3
Evaluate the limit of t t by plugging in 0 0 for t t.
0⋅e 0+e 0−e lim t→0 t 0⋅e 0+e 0-e lim t→0t
Step 3.4
Evaluate the limit of t t by plugging in 0 0 for t t.
0⋅e 0+e 0−e 0 0⋅e 0+e 0-e 0
0⋅e 0+e 0−e 0 0⋅e 0+e 0-e 0
Step 4
Simplify the answer.
Tap for more steps...
Step 4.1
Simplify the numerator.
Tap for more steps...
Step 4.1.1
Anything raised to 0 0 is 1 1.
0⋅1+e 0−e 0 0⋅1+e 0-e 0
Step 4.1.2
Multiply 0 0 by 1 1.
0+e 0−e 0 0+e 0-e 0
Step 4.1.3
Anything raised to 0 0 is 1 1.
0+1−e 0 0+1-e 0
Step 4.1.4
Add 0 0 and 1 1.
1−e 0 1-e 0
1−e 0 1-e 0
Step 4.2
Anything raised to 0 0 is 1 1.
1−1⋅1 1-1⋅1
Step 4.3
Multiply−1-1 by 1 1.
1−1 1-1
Step 4.4
Divide 1 1 by −1-1.
−1-1
−1-1
lim t→0(t e t 1−e t)lim t→0(t e t 1-e t)
lim t→0(t e t 1−e t)t lim t→0(t e t 1-e t)t lim t→0(t e t 1−e t)t 2 lim t→0(t e t 1-e t)t 2 lim t→0(t e t 1−e t)t 3 lim t→0(t e t 1-e t)t 3
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11366 | https://alg.manifoldapp.org/read/introduction-to-cartography/section/c3c06272-8b8b-49e7-a957-da0d06550b73 | Chapter 3 Part 1 - Choropleth Maps | Introduction to Cartography | OpenALG
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Introduction to Cartography: Chapter 3 Part 1 - Choropleth Maps
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Chapter 3 Part 1 - Choropleth Maps
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table of contents
1. Chapter 1 - Introduction to Cartography
1. Chapter 1 - Introduction to Cartography
2. 1.1 - Defining a Map
3. 1.2 - Classifying Maps
4. 1.3 - Categories of Thematic Maps
5. 1.4 - Taxonomy of Maps
6. 1.5 - Cartography
7. 1.6 - A Brief History of Maps
8. Other Resources
9. Summary
10. Credits
Chapter 2 - Map Elements and Design Principles
Chapter 2 - Map Elements and Design Principles
2.1 - The Cartographic Process
2.2 - Element Considerations
2.3 - Planar and Hierarchical Organization on a Map
2.4 - Example Map Critique
Other Resources
Summary
Credits
Chapter 3 Part 1 - Choropleth Maps
Chapter 3 Part 1 - Choropleth Maps
3.1 - Choropleth Maps
Other Resources
Summary
Credits
Chapter 3 Part 2 - Thematic Maps
Chapter 3 Part 2 - Thematic Maps
3.2 - Proportional Symbol Maps
3.3 - Dot Density Maps
Other Resources
Summary
Credits
Chapter 3 Part 3 - Other Map Types
Chapter 3 Part 3 - Other Map Types
3.4 - Cartograms
3.5 - Flow Maps
3.6 - Bivariate Mapping
Summary
Credits
Chapter 4 - Data for a Map
Chapter 4 - Data for a Map
4.1 - Data for a Mapping Project
4.2 - Normalization of Data
4.3 - Data Classification
Other Resources
Summary
Credits
Chapter 5 - Map Symboles, Visual Variables, Color
Chapter 5 - Map Symboles, Visual Variables, Color
5.1 - Map Symbols
5.2 - Spatial Arrangement
5.3 - Level of Measurement
5.4 - Visual Variables
5.5 - Color and Cartography
Other Resources
Summary
Chapter 6 Part 1 - Geodesy and Coordinate Systems
Chapter 6 Part 1 - Geodesy and Coordinate Systems
6.1 - What is Geodesy?
6.2 - Coordinate Systems
Other Resources
Summary
Chapter 6 Part 2 Map Projections
Chapter 6 Part 2 Map Projections
6.3 - Map Projections
6.4 - Map Projection Families
6.5 - Map Projection Properties
Other Resources
Summary
Credits
Chapter 6 Part 3 Map Projection Distortions
Chapter 6 Part 3 Map Projection Distortions
6.6 - Determining Distortions
6.7 - Map Projection Types
6.8 - Projected Coordinate Systems
Other Resources
Summary
Credits
Chapter 7 - Typography
Chapter 7 - Typography
7.1 - Introduction to Typography
Other Resources
Summary
Chapter 8 - Lying with Maps
Chapter 8 - Lying with Maps
8.1 - Little Lies
8.2 - Big Lies
Other Resources
Credits
About This Text
Chapter 3 Part 1 - Choropleth Maps | Introduction to Cartography | OpenALG
Chapter 3 - Part 1: Choropleth Maps
Uli Ingram
This chapter covers various types of maps and their features. Many types of maps exist so that cartographers can visualize spatial phenomenon in the most advantageous way. It is important that you be aware of all the different map types available to you so that you can visualize your data in the format that will be most appropriate for the content of your map and your map user. This chapter covers three map types: choropleth maps, proportional symbol maps, and dot-density maps. The first part of the chapter covers choropleth maps.
3.1: Choropleth Maps
A choropleth map is a map where colored or shaded areas represent the magnitude of an attribute. For example, this map shows the population density in the year 2007 for the United States of America. For each state, the number of persons per square mile has been calculated. The states with a lower population density are shaded with a lighter gray color. The states of a higher population density are shaded with a dark gray color. The states with population densities between the two extremes are shaded on a continuum from the lightest gray to the darkest gray. Based on the five different shades of gray, the map visually represents in an intuitive manner where the most densely populated states are in the United States.
Figure 1: Choropleth Map
Why Create a Choropleth Map? There are many reasons why you would want to create a choropleth map. Choropleth maps are relatively easy to create and easy to interpret by map readers. A choropleth map excels at displaying variables overall geographic pattern. As each color or shade is assigned a value or range of values the map reader can ascertain the values displayed on the map easily. Choropleth maps are also excellent for comparing multiple choropleth maps with one another to see how the spatial distribution of variable changes. We refer to multiple small maps on the same page as small multiples. A small multiple is when you have multiple small choropleth maps made with similar structure and context.
It is important that the only data represented on the choropleth map is data that can be linked to an enumeration area. An enumeration area is an area where data is collected and combined. Common enumeration areas in the United States are states, counties, and regions. It is important that the data be normalized against enumeration areas or a total population true blue area or size bias. What is meant by area or size bias is that larger areas might tend to have more population simply because there is more area for people to live? Smaller areas will naturally have less population because there is less area to live in.
By normalizing data against the enumeration area and taking size out of the equation you can do apple to apples comparisons between areas that have different sizes. Examples of normalized data are population per square mile which gives us population density, and percent unemployed which is the number of unemployed people divided by the total number of people eligible for work. In a choropleth map, the boundaries of areas do not have a related value. In other words, the outline of an area is in no way related to the value of the area. Only the different color or shaded the area is related to the value.
Inappropriate Data: There are several types of inappropriate data for choropleth mapping. Continuous data is not appropriate for inclusion on the choropleth map as continuous data is not controlled by an enumeration unit. For example, air temperature is not confined to County outlines nor is it logical to assume so. Another type of inappropriate data is any map ratio not involving an area. That means if a value can be assigned to a very specific point and it is not logical to aggregate that data value to a larger area, it should not be used for the choropleth map. Total values should not be used on a choropleth map. Variables, where the values vary too much, should also not be used for choropleth maps. If you still wish to use variables with a large value range you may want to consider choosing a smaller enumeration unit so that there is a smaller variation in each enumeration unit.
Data Classification: In order to display the vast majority of data on a choropleth map, you must employ some data classification schemes. We classify to simplify generalized the data for display on the map. In general, four to seven classes are preferred. If you need to exceed seven classes you need to keep in mind that humans cannot effectively use more than eleven classes at once. Now consider the five types of classification methods to determine when to use each one on a choropleth map. The equal-area data classification method is useful for layouts including multiple maps. The equal frequency data classification method is useful if you are performing a statistical test between classes. The arithmetic and geometric data classification methods are useful for the data that shows a normal distribution. The nested means data classification method is useful for non-normal distributions. And finally, the natural breaks data classification method maximizes homogeneity within classes and is typically going to be your best general choice for displaying data on a choropleth map.
Projection: In most cases for choropleth maps the equivalent, or equal area, projection are the most appropriate. The reason why the equal area map projections are the most appropriate is that since we typically normalize data based on area, relative size is important to maintain when comparing the values of the underlying enumeration.
Symbolization: Consider the symbolization choices for choropleth maps. If you are producing your choropleth map using black and white colors only, then the black color should represent larger values in the light grey color should represent smaller values. The color white should be generally reserved for the background of the map or outlines. Additionally, you should use caution with pure black and white fills as they may obscure boundary lines. You may use pattern, dot, line, or Hatcher patterns, instead of shades of gray, but this is considered to be the “old style” of choropleth mapping.
Black and White: Here is the population density choropleth map of the United States for the year 2007. In this black and white map the color white is used for the background and state outlines. The light gray color represents lower values and the dark gray color represents higher values.
Figure 2: Black and White Choropleth Map
Color: If you are producing your choropleth mapping color you should consider these points. Darker or more saturated colors represent larger values. Lighter or less saturated colors represent smaller values. Make sure you can easily differentiate between colors of different classes, that is, make sure that no two adjacent colors are too similar.
You should avoid qualitative color schemes on a quantitative choropleth map. That means, if you only have one variable on your map, such as population, you should choose a single color, or hue to represent that you are only showing different values of a single kind of thing. To represent the different quantities of that single thing, vary the saturation or value of the chosen color. On a color map, white suggests ‘light gray’ can effectively represent “no data”. Black or white is an effective boundary color on a color choropleth map.
On this color choropleth map that deals with a single variable of population, a single hue of green was chosen. The green hue is varied in saturation so that the lighter color green represents lower population density in the darker color green represents a higher population density. The color black was chosen as the state outlines as it provides great contrast against the green hue.
Figure 3: Color Choropleth Map
Color Schemes: In general, there are three color schemes that should be used on a color choropleth map based on the type of data being displayed. If your data is considered unipolar data, which means that there is no natural dividing point, you should use a sequential color scheme. An example of unipolar data is population density.
If you have bipolar data, which means that has a natural dividing point such as 0, or mean, then you should use diverging color scheme. Examples of bipolar data are population gains and losses. If you have balanced data, this means you have two complementary phenomena. In this case a diverging color scheme is appropriate. An example of this would be the ratio of males to females.
Reference Features: Thematic maps should be simple by design by focusing on the featured variable. When creating them you should avoid placing reference features on the map and less they are important in explaining the pattern of the variable being mapped.
Legend Design: To wrap up our discussion of choropleth maps this section will focus on legend design.
Legend Boxes: Choropleth maps typically use legend boxes. The legend boxes are typically square or rectangular and are large enough to provide a visual anchor but not too large to distract the eye from the main map body. The symbols in the legend should be identical to the symbols on the map in both color and line weight.
If the enumeration units on the map are reasonably small then the size of the symbol on the legend should be about the average size of the enumeration unit on the map. If the enumeration units on the map are very large then you may consider making the boxes ½ to 1/3 the average size of the enumeration unit on the map.
Figure 4: Legend Box
Legend Layout: The legend should be laid out into orientations: horizontally or vertically. With the horizontal orientation, the lowest value should be on the left and the highest value should be on the right. The value numbers should be located below the boxes. In a vertical layout you can either have the lowest or highest value on the top and the lowest or highest value on the bottom as neither layout, is considered standard. The numbers representing the value should be to the right of the boxes.
Figure 5: Horizontal Legend Box
Figure 6: Vertical Legend Box
Continuous Classes: In the case where the values on your map represent continuous data, which means that the maximum value in one class is slightly less than the minimum value of the next class, you should follow these guidelines. Your legend should emphasize the degradation of values and show that the values on the map exhaust the data. Additionally, the legend should reinforce the fact that there is no data that falls between the cracks. By having a continuous legend it allows the same legend to be applied to multiple maps. In our example, to reinforce the fact that the data is exhaustive and there are no cracks, the boxes of but each other and look like a single continuum.
Figure 7: Continuous Classes
Non-Continuous Classes: If you have non-continuous classes on your map then your legend should show the actual extreme values in each class. You would want to do this to narrow the reader’s estimate of the actual values in each class. A non-continuous legend is best with a single map displaying non-continuous data. For example, our legend shows each box separated from the other boxes to reinforce the fact the classes are not exhaustive and on a single continuum.
Figure 8: Non-Continuous Classes
Formatting Conventions: Use either “to” or “-“ between class ranges. If there are more than four numbers a value, use a comma after every third number left of the decimal value. If you choose to have a legend title, the legend title should match the topic of the map and should not use abbreviations including symbols.
You should place any ancillary text below the legend of the information will not fit into a concise legend title. If you are creating an animated map that shows the change of the variable throughout time, you should use a single continuous legend that encompasses the global maximum and global minimum over the entire series of the maps included in the animation.
Other Resources
Storymap about choropleth maps
Summary
This part of the chapter covered various types of maps and their features. This first part of the chapter focused on choropleth maps. You learned about appropriate and inappropriate data as well as data classifications and symbolization for each map type. Map legends and the elements that should be considered when using this feature were also covered.
Credits
This work by the National Information Security and Geospatial Technologies Consortium (NISGTC), and except where otherwise noted, is licensed under the Creative Commons Attribution 3.0 Unported License.
Authoring Organization: Del Mar College
Written by: Richard Smith
Copyright: © National Information Security, Geospatial Technologies Consortium (NISGTC)
Development was funded by the Department of Labor (DOL) Trade Adjustment Assistance Community College and Career Training (TAACCCT) Grant No. TC-22525-11-60-A-48; The National Information Security, Geospatial Technologies Consortium (NISGTC) is an entity of Collin College of Texas, Bellevue College of Washington, Bunker Hill Community College of Massachusetts, Del Mar College of Texas, Moraine Valley Community College of Illinois, Rio Salado College of Arizona, and Salt Lake Community College of Utah.
This workforce solution was funded by a grant awarded by the U.S. Department of Labor's Employment and Training Administration. The solution was created by the grantee and does not necessarily reflect the official position of the U.S. Department of Labor. The Department of Labor makes no guarantees, warranties or assurances of any kind, express or implied, with respect to such information, including any information on linked sites, and including, but not limited to accuracy of the information or its completeness, timeliness, usefulness, adequacy, continued availability or ownership.
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The x-intercepts of a quadratic equation are the values of x at which the function equals zero. These are also called the roots of the equation.
If you have a quadratic equation in the standard form:
a x 2+b x+c=0
The x-intercepts or roots can be found using the quadratic formula:
x=−b±b 2−4 a c 2 a
The term b 2−4 a c is known as the discriminant. It determines the number and type of solutions of a quadratic equation. If the discriminant is:
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11368 | http://ncvs2.books.nba.co.za/chapter/unit-3-mechanical-advantage-of-simple-machines/ | Unit 3: Mechanical advantage of simple machines – National Curriculum (Vocational) Physical Science Level 2
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I. Mechanics: Identify, describe and apply principles of motion in one dimension
Unit 1: Motion in one dimension
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Unit 2: Calculations on motion in one dimension
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Unit 3: The concepts of vectors and scalars
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Unit 1: What is a force?
Definition of force
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What is a force diagram?
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Unit 3: Mass and weight
Gravity
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III. Mechanics: Identify, describe and apply principles of mechanical energy
Unit 1: Introduction to mechanical energy
The concept of mechanical energy
Kinetic energy
Gravitational potential energy
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Unit 2: Conservation of mechanical energy
Mechanical energy
Conservation of energy
The law of conservation of mechanical energy
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IV. Mechanics: Identify, describe, and apply principles of simple machines and mechanical advantage in everyday contexts
Unit 1: Simple machines
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Unit 2: The concept of mechanical advantage
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Unit 3: Mechanical advantage of simple machines
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V. Waves, sound and light: Identify, describe and apply principles of waves
Unit 1: Properties of waves
What is a wave?
Properties of wave motion
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Unit 2: Types of waves
Different types of wave motion
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Unit 3: Wave calculations
Calculating the properties of a wave
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Unit 4: Standing waves
Standing waves in the world around us
The concept of standing waves
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VI. Waves, sound and light: Identify, describe and apply principles of geometrical optics in everyday contexts
Unit 1: Wave properties of light: Reflection and refraction
Light is a wave
Reflection
Refraction
Total internal reflection
Unit 1: Assessment
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Unit 2: More on reflection of light
An introduction to mirrors and images
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VII. Magnetism and electricity: Identify, describe and apply principles of magnetism
Unit 1: Magnets and magnetic fields
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Unit 2: The Earth’s magnetic field
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Unit 3: Magnetic shielding
Unit 3: Assessment
Unit 3: Solutions
VIII. Magnetism and electricity: Identify, describe, and apply principles of electrostatics (static electricity)
Unit 1: What is charge?
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Interaction of charge
Unit 2: Assessment
Unit 2: Solutions
Unit 3: Electrostatics in practice
Unit 3: Assessment
Unit 3: Solutions
IX. Magnetism and electricity: Identify, describe and apply properties of electricity in an electric circuit
Unit 1: Electric current
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Resistance in an electric circuit
Unit 2: Assessment
Unit 2: Solutions
Unit 3: Voltage in an electric circuit
Unit 3: Assessment
Unit 3: Solutions
Unit 4: Safety with electricity
Unit 4: Assessment
Unit 4: Solutions
X. Matter and materials: Identify, describe, and classify matter according to different macroscopic properties
Unit 1: Phases of matter
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Properties of Materials
Unit 2: Assessment
Unit 2: Solutions
XI. Matter and materials: Identify and describe atoms as the basic building block
Unit 1: The atom
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Atomic number and atomic mass
Unit 2: Assessment
Unit 2: Solutions
XII. Matter and materials: Identify, describe and apply properties of the periodic table
Unit 1: The periodic table
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Electron configuration
Electron configuration
Unit 2: Assessment
Unit 2: Solutions
Unit 3: The behaviour of elements in specific groups
Unit 3: Assessment
Unit 3: Solutions
XIII. Matter and materials: Identify and describe particles
Unit 1: Particles
Atoms
Molecules
Unit 1: Assessment
Unit 2: Solutions
Unit 2: Elements, mixtures, and compounds
Unit 2: Assessment
Unit 2: Solutions
Unit 3: Bonding
Chemical bonding
Writing chemical formulae
Unit 3: Assessment
Unit 3: Solutions
XIV. Chemical change: Identify, describe, and apply principles of heat
Unit 1: First law of thermodynamics
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Heat and heat transfer
Unit 2: Assessment
Unit 3: Specific heat capacity
Unit 3: Assessment
Unit 3: Solutions
XV. Chemical change: Differentiate between physical and chemical change
Unit 1: Chemical and physical change
Physical changes
Chemical changes
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Separating mixtures
Separating mixtures
Unit 2: Assessment
Unit 2: Solutions
XVI. Chemical change: Identify, describe, and apply principles of chemical reactions (electrolytes)
Unit 1: Principles of chemical reactions
Unit 1: Assessment
Unit 1: Solutions
XVII. Chemical change: Determine the quantitative aspects of change
Unit 1: Quantitative aspects of change
Unit 1: Assessment
Unit 1: Solutions
XVIII. Chemical systems and industry: Identify and describe the impact of scientific knowledge of the hydrosphere on the quality of human, environmental, and socio-economic development
Unit 1: The hydrosphere
The hydrosphere
Unit 1: Assessment
Unit 1: Solutions
Unit 2: Water pollution
Unit 2: Assessment
Unit 2: Solutions
Unit 3: Treatment and purification of potable water
Unit 3: Assessment
Unit 3: Solutions
National Curriculum (Vocational) Physical Science Level 2
Mechanics: Identify, describe, and apply principles of simple machines and mechanical advantage in everyday contexts
Unit 3: Mechanical advantage of simple machines
Leigh Kleynhans
Unit outcomes
By the end of this unit you will be able to:
Define ideal mechanical advantage (IMA) as the ratio between the distance through which the effort force moves an object and the distance through which the resistance force moves an object: IMA = distance effort force ÷ distance resistance force.
Define actual mechanical advantage (AMA) as the ratio between the resistance force and the effort force: AMA = resistance force ÷ effort force.
Calculate the relative efficiency of a simple machine: efficiency (%) = (AMA ÷ IMA) x 100 100.
What you should know
Before you start this unit, make sure you can:
Identify levers as simple machines, as covered in Subject outcome 2.4, Unit 1.
Calculate mechanical advantage, as covered in Subject outcome 2.4, Unit 2.
Introduction
In the previous unit, you learnt to calculate the mechanical advantage of levers as simple machines. These calculations are theoretical and do not take friction, flexing or wear-and-tear into account. In this unit we will learn how these factors can affect the output of a simple machine. We will also learn about the difference between ideal mechanical advantage (IMA) and actual mechanical advantage (AMA), and how to apply your knowledge to calculate the efficiency of various simple machines.
Ideal mechanical advantage
The ideal mechanical advantage (IMA) is the mechanical advantage of a device with the assumption that its components do not flex, there is no friction, and there is no wear-and-tear. It is calculated using the physical dimensions of the device and defines the maximum performance the device can achieve. It is a theoretical value calculated using the formula:
I M A=d e d r I M A=d e d r
where:
d e d e is the distance of the effort force
d r d r is the distance of the resistance force
In reality, a machine will dissipate energy to overcome friction as surfaces move over each other causing wear-and-tear, heat, and sound. This calculation will therefore not reflect the actual output of the machine.
Example 3.1
A box is lifted using a lever. The distance of the box from the fulcrum is 1.5 m 1.5 m and the effort force is applied at 2.5 m 2.5 m from the fulcrum. Calculate the ideal mechanical advantage of this simple machine.
Solution
Step 1: Write the formula for ideal mechanical advantage
I M A=d e d r I M A=d e d r
Step 2: Substitute the given values
I M A=2.5 1.5 I M A=2.5 1.5
Step 3: Write the answer
I M A=1.67 I M A=1.67
Actual mechanical advantage
Actual mechanical advantage (AMA) is calculated using actual measurements of the output of a machine. The actual mechanical advantage will always be less than the ideal mechanical advantage. The formula used for actual mechanical advantage is:
A M A=F r F e A M A=F r F e
where:
F r F r is the resistance force
F e F e is the effort force
Example 3.2
A box of mass 500 kg 500 kg is lifted using a lever. The applied force is 3 000 N 3 000 N. Calculate the actual mechanical advantage of this simple machine.
Solution
Step 1: Calculate the resistance force
This is the weight of the box
F g=m g= 500 x 9.8= 4 900 N F g=m g= 500 x 9.8= 4 900 N
Step 2: Write the formula for actual mechanical advantage
A M A=F r F e A M A=F r F e
Step 3: Substitute the given values
A M A=4 900 3 000 A M A=4 900 3 000
Step 4: Write the answer
A M A=1.63 A M A=1.63
Efficiency of simple machines
Efficiency is a measure of how well a machine can perform. To calculate the efficiency of a machine, we look at the ratio of the actual mechanical advantage to the ideal mechanical advantage and then convert it to a percentage:
efficiency =A M A I M A x 100 efficiency =A M A I M A x 100
A high percentage efficiency indicates a machine with a high output and little energy ‘lost’ to heat or sound. Whereas a machine with a low percentage efficiency will have a low output with much energy transformed into heat or sound.
Example 3.3
A box with a weight of 2 500 N 2 500 N is placed at a distance of 1.25 m 1.25 m from the fulcrum of a lever. It is lifted using an applied force of 1 3 00 N 1 3 00 N acting at 2.75 m 2.75 m from the fulcrum at the other end of the lever. Calculate the efficiency of this simple machine.
Solution
Step 1: Calculate the actual mechanical advantage
A M A=F r F e=2 500 1 300= 1.92 A M A=F r F e=2 500 1 300= 1.92
Step 2: Calculate the ideal mechanical advantage
I M A=d e d r=2.75 1.25= 2.2 I M A=d e d r=2.75 1.25= 2.2
Step 3: Write formula for efficiency of simple machines
efficiency =A M A I M A x 100 efficiency =A M A I M A x 100
Step 4: Substitute values
efficiency =1.92 2.2 x 100 efficiency =1.92 2.2 x 100
Step 5: Write the answer
87.27%87.27%
Summary
In this unit you have learnt the following:
Machines do not produce a theoretical output because not all energy is transformed into useful work during their operation.
Ideal mechanical advantage (IMA) is the theoretical calculation of the maximum possible output of a machine.
Actual mechanical advantage (AMA) is the measurement of the actual output of the machine.
Actual mechanical advantage will always be less than ideal mechanical advantage because some work is done to overcome friction and is transformed into heat and sound.
Efficiency is an indication (in a percentage) of the ratio between the IMA and the AMA.
Unit 3: Assessment
Suggested time to complete: 15 minutes
In an acrobatic demonstration, one person jumps onto the end of a plank (lever). This creates a large effort force of magnitude 9.2 x 1 0 2 N 9.2 x 1 0 2 N at the end of the board at a distance of 1.7 m 1.7 m from the fulcrum. A smaller person (with a load force of 4.6 x 1 0 2 N 4.6 x 1 0 2 N) located 3.1 m 3.1 m away from the fulcrum) moves a larger distance and high enough to perform acrobatic moves.
.
Calculate:
1. the AMA of the board
2. the IMA of the board
3. the efficiency of the system.
The input force of 15 N 15 N acting on the effort arm of a lever moves 0.4 m 0.4 m. This lifts a 40 N 40 N weight, resting on the resistance arm, a distance of 0.1 m 0.1 m
Explain why the AMA of a machine is generally less than its IMA.
What is the efficiency of the machine?
A wheelbarrow is 75 75 efficient. Use the information in the diagram to calculate the mass of the load in the wheelbarrow.
The full solutions are at the end of the unit.
Unit 3: Solutions
Unit 3: Assessment
.
F e=9.2 x 1 0 2 N d e=1.7 m F r=4.6 x 1 0 2 m d r=3.1 m F e=9.2 x 1 0 2 N d e=1.7 m F r=4.6 x 1 0 2 m d r=3.1 m
1. A M A=F r F e=4.6 x 1 0 2 9,2 x 1 0 2=0.5 A M A=F r F e=4.6 x 1 0 2 9,2 x 1 0 2=0.5
2. I M A=d e d r=1.7 3.1=0.55 I M A=d e d r=1.7 3.1=0.55
3. E f f i c i e n c y=A M A I M A x 100 =0.5 0.55 x 100 = 91%E f f i c i e n c y=A M A I M A x 100 =0.5 0.55 x 100 = 91%
.
F e=15 N d e=0.4 m F r=40 N d r=0.1 m F e=15 N d e=0.4 m F r=40 N d r=0.1 m
1. Not all the input energy is converted to output energy. Some energy is transformed to heat and sound because of friction.
2. A M A=F r F e=40 15=2.67 A M A=F r F e=40 15=2.67
I M A=d e d r=0.4 0.1=4 I M A=d e d r=0.4 0.1=4
E f f i c i e n c y=A M A I M A x 100=2.67 4 x 100 = 67%E f f i c i e n c y=A M A I M A x 100=2.67 4 x 100 = 67%
I M A=d e d r=1.2 0.5=2.4 I M A=d e d r=1.2 0.5=2.4
E f f i c i e n c y=A M A I M A x 100 75 =A M A 2.4 x 100 A M A= 1.8 E f f i c i e n c y=A M A I M A x 100 75 =A M A 2.4 x 100 A M A= 1.8
.
A M A=F r F e 1.8=F r 200 F r=360 N A M A=F r F e 1.8=F r 200 F r=360 N
.
F g=m g 360=m x 9.8 m=36.73 kg F g=m g 360=m x 9.8 m=36.73 kg
Back to Unit 3: Assessment
Media Attributions
img03_AssessmentQ3 © DHET is licensed under a CC BY (Attribution) license
a theoretical calculation based on the dimensions of the machine that gives the maximum possible output of a machine
an actual indication of the performance of a machine, the ratio between the resistance force and the effort force
a percentage that indicates the comparison between the input and the output of a machine
Previous: Unit 2: The concept of mechanical advantage
Next: Waves, sound and light: Identify, describe and apply principles of waves
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National Curriculum (Vocational) Physical Science Level 2 by Leigh Kleynhans is licensed under a Creative Commons Attribution 4.0 International License, except where otherwise noted.
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11369 | https://www.medicalnewstoday.com/articles/319941 | Heliotrope rash: Causes, pictures, and treatment
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What is a heliotrope rash?
Medically reviewed by Nancy Carteron, M.D., FACR — Written by Zawn Villines — Updated on July 14, 2023
What are the causes and risk factors?
Symptoms
Diagnosis and when to see a doctor
Treatment
Takeaway
A heliotrope rash is a reddish purple rash on or around the eyelids. It can look patchy and may accompany a swollen eyelid. It is a characteristic of dermatomyositis. Other risk factors include autoimmune conditions, infections, and more.
A heliotrope rash is a reddish purple rash that occurs as the first noticeable symptom of an inflammatory muscle disease called dermatomyositis. The rash takes its name from the heliotrope flower, which has purple petals.
Dermatomyositis causes progressive muscle weakness. In children, it can also damage the blood vessels.
What are the causes and risk factors?
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The heliotrope rash can appear uneven and may be combined with a swollen eyelid.
A heliotrope rash is characteristic of dermatomyositis. Dermatomyositis is part of a group of muscle diseases called inflammatory myopathies or myositis (inflammation of muscle).
Dermatomyositis is a chronic autoinflammatory disease, with symptoms that may change over time. About a third of people Trusted Source who develop dermatomyositis as children recover, but the remainder continue to experience symptoms.
Researchers are unsure what causes dermatomyositis. It may be due to an underlying genetic predisposition that is triggered by a bacteria, virus, or even sunlight. Dermatomyositis is rare, affecting less than 10 out of every million people.
Women are twice as likely to get dermatomyositis as men. While it is possible to develop this condition at any age, it is more prevalent among children aged 5 to 10. Juvenile dermatomyositis affects children and can cause damage to the blood vessels as well as muscle weakness.
Other risk factors for dermatomyositis and the heliotrope rash that accompanies it include:
cancer, particularly in older people (paraneoplastic syndrome)
an autoimmune disorder or a predisposition to autoimmune diseases
medications, infections, or injuries
a viral infection
sunburn or heavy sun exposure
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Symptoms
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A heliotrope rash is the first noticeable symptom of dermatomyositis. Image credit: Elizabeth M. Dugan, Adam M. Huber, Frederick W. Miller, Lisa G. Rider, 2010.
The heliotrope rash may be uneven and bumpy and often looks dry and irritated. It may burn or itch, or it may cause no symptoms other than reddened skin. In most people with dermatomyositis, a heliotrope rash appears before the muscular symptoms.
Over time, other symptoms may appear. In addition to skin lesions, flaky spots on the elbows and knees, and a rash on the knuckles, other signs of dermatomyositis include:
Progressively worsening muscle weakness, particularly in the upper arms and upper thighs. Some people initially notice difficulty getting up from a seated position, or have trouble combing their hair.
Sudden muscle weaknesses in the hips, back, or shoulders.
Swelling and redness around the fingernails.
Hard lumps under the skin, which are due to calcium deposits under the skin.
Feelings of exhaustion and weakness.
Difficulty swallowing, including sensations of choking or a lump in the throat.
A hoarse voice that may accompany swallowing problems.
Muscle pain, though not all people with dermatomyositis develop muscle pain.
People with dermatomyositis may be more vulnerable to a lung disorder called interstitial lung disease. This disease damages lung tissue and can make it difficult to breathe. Some people with interstitial lung disease develop lung stiffness and weakness.
The presence of specific antibodies in the blood may make it more likely that a person will develop interstitial lung disease.
Diagnosis and when to see a doctor
It is not possible to self-diagnose dermatomyositis based solely on the presence of a rash.
It can mimic some other conditions. Moreover, a rash on or around the eyes can pose a threat to vision, so it is vital to get an accurate diagnosis.
People who develop a painful or itchy rash on the eyes should see a doctor promptly, especially if the eyelids are swollen. If the eyelid is red or inflamed, but not painful, it is fine to wait for 1 to 2 days.
If the rash does not disappear, however, see a doctor. If an eyelid rash occurs along with other symptoms of dermatomyositis, ask a doctor for a referral to a specialist doctor, usually a rheumatologist.
Treatment may begin by ruling out other conditions, such as pink eye, an allergic reaction, or an injury to the eyelid. Other disorders that may cause a rash on the eye include lupus, HIV, and an inflammatory skin condition called lichen planus.
Diagnosing dermatomyositis can be difficult, so it is important to work with a dermatologist. Diagnostic tests may include:
Blood tests: These can detect enzymes and autoantibodies associated with dermatomyositis and other muscle or neurological disorders.
Biopsy: A biopsy of the rash, or of other irritated or inflamed areas of the skin. A biopsy removes a small sample of tissue, which is then stained and examined under a microscope.
Imaging tests: Such as magnetic resonance imaging (MRI) of the muscles. These tests can show signs of muscle inflammation, even when a person has not yet experienced muscle weakness.
Nerve conduction and EMG (electromyograms): These can also show early signs of muscle weakness, but they involve placing needles in the muscles, which can be painful.
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Treatment
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Dermatomyositis pain may be improved with chiropractic therapies or massage.
There is no cure for dermatomyositis, though symptoms may get better or even go away on their own. The right treatment depends on symptoms, the person’s overall health, and the specific antibodies present in their blood. Some treatment options include:
Corticosteroid drugs: Topical lotions can help with itching and other skin symptoms. Systemic corticosteroids may suppress the immune system and prevent dermatomyositis from getting worse.
Immunosuppressants: These are drugs that block activity in the immune system. Because dermatomyositis may be due to an overactive immune system, most people see an improvement in their symptoms. Immunosuppressants can put a person at risk of infections, however, so taking these drugs will depend on the person’s overall health.
Physical and exercise therapy: This can help resolve the symptoms by stimulating the affected area and maintaining a person’s range of motion.
Devices to support and assist the muscles: If the foot muscles become weak, a splint or shoe insert may help.
Heat therapy: That can reduce inflammation in the muscles by increasing blood flow.
Complementary therapies: Such as massage, acupressure, and chiropractic therapies can reduce pain.
»MORE:Get a skin condition evaluation in as little as 15 minutes with Optum Now Online Care.
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Takeaway
A heliotrope rash is not dangerous, but it does point to a potentially serious underlying condition. Proper diagnosis can rule out cancer, which will need to be treated before dermatomyositis.
Prompt treatment can improve outcomes in people with dermatomyositis, making it possible to lead a normal life with minimal muscle weakness.
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From preventive treatments to clever cleaning hacks and wardrobe choices, there's many ways to manage flaking. Read on for some effective tips to make living with psoriasis more comfortable and flake-free.
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Dermatology
Eye Health / Blindness
How we reviewed this article:
Sources
Medical News Today has strict sourcing guidelines and relies on peer-reviewed studies, academic research institutions, and medical journals and associations. We only use quality, credible sources to ensure content accuracy and integrity. You can learn more about how we ensure our content is accurate and current by reading oureditorial policy.
Dermatomyositis. (2015, January)
Diagnosis. (2015, March)
Inflammatory myopathies. (2017, March)
Inflammatory myopathies fact sheet. (n.d.)
Interstitial lung disease. (2014, March)
Koler, R. A., & Montemarano, A. (2001, November 1). Dermatomyositis.American Family Physician,64(9), 1565–1573
Miller, M. (2017, March 13). Patient education: Polymyositis, dermatomyositis, and other forms of idiopathic inflammatory myopathy. (Beyond the basics)
Polymyositis/dermatomyositis. (2012, March)
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Medically reviewed by Nancy Carteron, M.D., FACR — Written by Zawn Villines — Updated on July 14, 2023
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11370 | https://www.phyley.com/mass-hanging-from-two-ropes | Problem: A mass hanging from two ropes
A mass of 108 g is hanging from two massless ropes attached to the ceiling.
One rope makes an angle of 50° with the ceiling, while the other makes an angle of 29°.
Find the tensions in the two ropes.
Solving the problem
Let's begin by drawing our mass hanging from the two ropes:
Looking at our sketch, we can infer that the mass is subject to 3 forces:
Here's the free-body diagram of our hanging mass:
We know the mass (108 g, which in kilograms is 0.108 kg), and the angles that the two ropes make with the ceiling (50° and 29°).
We are asked to find the tensions in the two ropes.
We know
We want to know
The mass is hanging.
What does this tell us?
This tells us that the acceleration of the mass must be zero.
And because the acceleration is zero, the resultant force acting on the mass is also zero. Indeed, for Newton's 2nd Law:
Now that we determined that the resultant force acting on the mass is zero, we can find the tensions of the two ropes using the following step by step process:
Let's start with the first step.
We draw the coordinate axes on our free-body diagram. For convenience, we choose the x axis horizontal and the y axis vertical. Then, we determine the x and y components of all the forces that act on the mass.
We need to keep in mind that the angle between each tension force and its x component is equal to the angle that the rope, producing that tension, makes with the ceiling:
Thus, the x and y components of the resultant force will be:
x:
y:
The next step is to substitute Rx and Ry in Eq. (1) and Eq. (2) with 0:
Using these two equations we can easily find T1 and T2.
There are multiple ways in which we can do this. One way would be to first solve Eq. (3) for T2:
T2=T1 | cos50°
cos29°
Then, we substitute T2 with 0.735T1 in Eq. (4):
And we solve it for T1:
T1= | mg
1.12
T1= | (0.108kg) (9.81N/kg)
1.12
Finally, we substitute the value of T1 in Eq. (5) to find T2:
Therefore, the tension in the rope at the 50° angle is 0.946 N, and the tension in the rope at the 29° angle is 0.695 N.
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11371 | https://www.quora.com/What-is-the-difference-between-subsequence-substrings-and-subarrays-In-competitive-programming-I-see-so-many-questions-based-on-these-topics-Is-there-any-material-that-explains-the-difference-between-the-three-that | Something went wrong. Wait a moment and try again.
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What is the difference between subsequence, substrings, and subarrays? In competitive programming, I see so many questions based on these topics. Is there any material that explains the difference between the three that can help me to get started?
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Subsequence is what you get when you remove zero or more elements from your sequence/array/string and take what is left without changing order: Subsequence - Wikipedia.
Subarray is a block of contiguous elements from your array. Every subarray is also a subsequence, because you can get it by removing all the elements before and after this subarray - but not every subsequence is a subarray, because a subsequence does not necessarily consist of contiguous elements. In some badly prepared problems you may find authors mistakenly using word subsequence to describe subarray - especially if they aren
Subsequence is what you get when you remove zero or more elements from your sequence/array/string and take what is left without changing order: Subsequence - Wikipedia.
Subarray is a block of contiguous elements from your array. Every subarray is also a subsequence, because you can get it by removing all the elements before and after this subarray - but not every subsequence is a subarray, because a subsequence does not necessarily consist of contiguous elements. In some badly prepared problems you may find authors mistakenly using word subsequence to describe subarray - especially if they aren’t native English speakers, and terminology works differently in their language.
Substring is the same as subarray, but defined on strings. You take any piece of original string - and that’s your substring. See Substring - Wikipedia.
It’s hard to call it topics - these are simply terms used to describe very fundamental (and common) concepts. You won’t be able to find any guide on how to solve problems on subarrays, because there are lots and lots of classes of problems that use subarrays in one way or another, and they don’t have too much in common. Problems that ask you to answer some queries on subarrays are usually significantly different from problems that ask you to count subarrays, which are in turn different from problems that ask you to find some subarray with special properties.
Hopefully this answer will be sufficient to understand the difference between subsequence, substring, and subarray. It won’t automatically make you able to solve problems though - in order to get there you’ll need to patiently practice problem solving.
Daniel R. Page
Theoretical Computer Scientist, CS PhD
·
Author has 3K answers and 5.2M answer views
·
5y
I will only address the first question (and will provide example problems using each concept):
Subarray - A subset of the elements of an array, typically elements are required to be contiguous (by index). E.g. Maximum subarray problem - Wikipedia [ ].
Substring - A substring of a string, every symbol is contiguous in a substring. E.g. Lon
I will only address the first question (and will provide example problems using each concept):
Subarray - A subset of the elements of an array, typically elements are required to be contiguous (by index). E.g. Maximum subarray problem - Wikipedia [ ].
Substring - A substring of a string, every symbol is contiguous in a substring. E.g. Longes...
Assistant
Bot
·
1y
Understanding the differences between subsequences, substrings, and subarrays is fundamental in competitive programming and algorithm design. Here’s a breakdown of each term:
Subsequence
Definition: A subsequence is a sequence derived from another sequence where some elements may be deleted without changing the order of the remaining elements.
Example: For the sequence ABC, the subsequences include A, B, C, AB, AC, BC, and ABC. The empty sequence is also considered a subsequence.
Key Point: Subsequences do not require elements to be contiguous.
Substring
Definition: A substring is a contiguous
Understanding the differences between subsequences, substrings, and subarrays is fundamental in competitive programming and algorithm design. Here’s a breakdown of each term:
Subsequence
Definition: A subsequence is a sequence derived from another sequence where some elements may be deleted without changing the order of the remaining elements.
Example: For the sequence ABC, the subsequences include A, B, C, AB, AC, BC, and ABC. The empty sequence is also considered a subsequence.
Key Point: Subsequences do not require elements to be contiguous.
Substring
Definition: A substring is a contiguous sequence of characters within a string.
Example: For the string ABC, the substrings include A, B, C, AB, BC, and ABC. The empty substring is also considered.
Key Point: Substrings must be contiguous and can only be derived from strings.
Subarray
Definition: A subarray is a contiguous segment of an array (similar to a substring in a string).
Example: For the array [1, 2, 3], the subarrays include , , , [1, 2], [2, 3], and [1, 2, 3].
Key Point: Like substrings, subarrays must be contiguous and can only be derived from arrays.
Summary of Differences
Contiguity:
Subsequence: Not required to be contiguous.
Substring: Must be contiguous.
Subarray: Must be contiguous.
Data Structure:
Subsequence: Can be derived from any sequence (arrays, strings, etc.).
Substring: Specific to strings.
Subarray: Specific to arrays.
Recommended Material to Get Started
Here are some resources that can help you understand these concepts better:
Online Tutorials:
GeeksforGeeks has great articles explaining these concepts with examples and code snippets. Look for articles on subsequences, substrings, and subarrays.
Competitive Programming Books:
"Introduction to Algorithms" by Cormen, Leiserson, Rivest, and Stein has sections that cover dynamic programming problems related to these topics.
"Competitive Programming" by Halim and Halim also includes problems and explanations related to subsequences and substrings.
Coding Platforms:
Websites like LeetCode, HackerRank, and Codeforces often have problems specifically focusing on these concepts. Look for tags related to dynamic programming and string manipulation.
YouTube Tutorials:
Search for videos on subsequences, substrings, and subarrays. Many competitive programming channels explain these concepts with visual aids and coding examples.
Practice Problems
To solidify your understanding, try solving problems related to:
- Longest common subsequence.
- Finding all substrings of a given string.
- Maximum sum subarray (Kadane’s Algorithm).
By practicing these concepts, you’ll gain a deeper understanding of how to manipulate and analyze sequences in competitive programming.
Related questions
What is difference between subarray and contiguous subarray?
In programming, how are subsets, subarrays, and subsequences different?
What is the difference between subString() and subSequence()?
What is the difference between a competitive problem and an interview problem in coding?
What is the difference between constructive questions and other questions at Codeforces (programming competitions)?
Kunal Verma
ICPC'20 World Finalist
·
Updated 2y
Related
How did you start competitive programming?
I started competitive coding in the first week of my college. It was the “interaction month” and one senior summoned me at his room. I turned up at his room with another guy who I had barely made friends with at that time. I was super scared, after the rumours I had heard about my other batchmates' “interactions” with seniors. This senior however turned out to be nothing like that and made us SIT and just talked to us. He then went on and explained us what CP is. It seemed challenging but I and the guy who tagged along liked the idea. 2 years down the line, that senior has been like a brother
I started competitive coding in the first week of my college. It was the “interaction month” and one senior summoned me at his room. I turned up at his room with another guy who I had barely made friends with at that time. I was super scared, after the rumours I had heard about my other batchmates' “interactions” with seniors. This senior however turned out to be nothing like that and made us SIT and just talked to us. He then went on and explained us what CP is. It seemed challenging but I and the guy who tagged along liked the idea. 2 years down the line, that senior has been like a brother to me who helps me keep my feet on the ground and has guided me through some tough times.
I and my friend decided to be CP buddies then. We started learning basic Data Structures like stacks and queues from hackerrank, and solved problems. I still remember seeing the difference array trick and being blown away by the genius of it :p
After just 15 days, there was a contest for freshers in the college. I was really excited and did well beyond my expectations, finishing third among the freshers. My confidence was sky high.
One month later, we had inductions for the programming club. It had several ICPC regionalists, including the senior who mentored me on the first day. It was a club of stature, and naturally seemed daunting. The contest happened and I got a rank of 27 out of 50 participants and was devastated. This was my first reality check. I and my friend swore to work hard and make it in the next inductions.
We started giving contests on Codeforces and Codechef. I remember the thrill and agony of waiting for the verdict on the screen during my first few contests :P. It was amazing. The adrenaline rush was real.
I and the guy who tagged along had become addicted to CP by the end of first sem. We were best friends by now and would do anything and everything together. Heck, we even skipped the Amit Trivedi concert in our college on our cultural fest for a lunchtime contest :P.
Second semester arrived soon. I had done considerable CP by now and had reached a rating of 1700 on Codeforces. Programming club inductions arrived again but getting inducted into the club wasn't the goal anymore. It had changed to coming first in the contest. I ended up getting 3rd place in college and was 1st among the freshers. I finally got inducted and felt on top of the world. My friend didn't (but he got inducted next year so it's okay :p).
Two years down the line in college now, the club getting into which seemed like an impossible task has now become a family away from home. I even got the honour to be appointed as the secretary of the club.
CP has given me a lot. It gave me the chance to experience unforgettable events like the ACM ICPC'19 regionals, Topcoder Open Indian Regionals '19 and Topcoder Humblef00l Cup '18, and that feeling of crossing 1900 rating for the first time :p are somethings that I'll treasure for my life. It has given me the chance to interact, compete and make friends with some of the most talented and intelligent people around the country. It has given me the chance to get to know some very wise seniors who've helped me in CP and with life in general. It has given some exceptionally talented teammates. It has made me a more determined and driven person. It has given me a chance to prove my worth to myself, when I felt like I had failed after failing to get CS in a top IIT. And it has given me a best friend. :)
Rajat Kumar
Programmer java , python , Ds and Algo expert
·
Upvoted by
Dharmendra
, B.Tech. Computer Science, IEC College of Engineering and Technology (2019) and
Vishal Chincholi
, B.E Computer Science, JSS Science and Technology University, Mysuru (2021) · Author has 69 answers and 2.5M answer views
·
Updated 5y
Related
How should I get started in competitive programming?
If you Actually want start competitive coding then you must have to follow this method.
Step 1
Learn C++ or Java. If you can learn C, you can learn C++ and I recommend java first.
Why? Because C++ and Java both works on object oriented programming also these are not too complex languages.
Again,
don't use Python, Ruby, etc, for CP. These are very high-level languages that won't give you as much control over your code as needed.
Step 2
Get on Hackerrank because it has the best User Interface, combined with relative ease of getting started for the beginners.
Ease in the sense that anyone with zero CP/al
If you Actually want start competitive coding then you must have to follow this method.
Step 1
Learn C++ or Java. If you can learn C, you can learn C++ and I recommend java first.
Why? Because C++ and Java both works on object oriented programming also these are not too complex languages.
Again,
don't use Python, Ruby, etc, for CP. These are very high-level languages that won't give you as much control over your code as needed.
Step 2
Get on Hackerrank because it has the best User Interface, combined with relative ease of getting started for the beginners.
Ease in the sense that anyone with zero CP/algorithms experience will be able to solve the beginner Questions because it’s for everyone.
You might get stuck after first 4-5 questions and that's normal. In that case, feel free to see the editorial or google to look for the solution.
When you find it, make sure to understand it, and then code it on your own.
First, solve "Easy" questions of all sections, and then "Medium" questions.
In fact, solving some "Medium" questions is good enough to call yourself a CP professional.
And when you make sure that you’re able to solve Medium questions , then start CP on CodeChef that is a much professional practical area to code.
Step 3
Codechef long contests are the best. Developing your Competitive Programming skills requires that you are both fast and are able to think deeply about a problem.
Codechef long challenges = Deep thinking AND Codeforces rounds = Fast coding
If you want to be good, you should try to be good in both these areas.
But it's fine if you are just good at long challenges (deep thinking) or just good with short contests (fast thinking), both will help you become a better programmer.
Step 4
You can try Topcoder if you want. Or just let it be.
With CP, if your goal is to get offers from Google HQ and likes, you will have to do it regularly. That is, give contests, try to rank higher, and build your rating.
Otherwise, you can just do it on the side and focus on building other practical skills.
These practical skills combined with your decent competitive programming experience will go a long way in helping you secure those jobs and internships you dreamed about.
Step 5
Keep doing this it will take Some time but it is the best way to be a Competitive Programmer.
Don’t Be Frustrated.
I need Your upvote ,
Hit up if you’re also think Programming is Best <3
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Kalpit Veerwal
Entrepreneur, IIT Bombay CSE '21, JEE 2017 AIR 1
·
Upvoted by
Krishna Kanna
, B.E Computer Science, Sri Sivasubramaniya Nadar College of Engineering, Tamil Nadu, India (2022) and
Prashant Singh
, MS Computer Science, University of Southern California (2023) · Author has 363 answers and 26.1M answer views
·
5y
Related
How should I get started in competitive programming?
Here's how I did:
Learn one programming language really well - preferably C++. Make sure you're super comfortable with all the constructs and can code up any algorithm given the pseudo code.
Go to Hackerrank. Easy problems for starters and a good UI. Get a badge or two in C++ and Problem Solving (5 stars in Hackerrank is not too tough to get).
Then go to SPOJ. Sort the problems in descending order of “number of people who have solved them”. This is important as it will make sure the problem level increases gradually. After 20–30 questions the problems tend to become quite tough. Solve 100.
This sh
Here's how I did:
Learn one programming language really well - preferably C++. Make sure you're super comfortable with all the constructs and can code up any algorithm given the pseudo code.
Go to Hackerrank. Easy problems for starters and a good UI. Get a badge or two in C++ and Problem Solving (5 stars in Hackerrank is not too tough to get).
Then go to SPOJ. Sort the problems in descending order of “number of people who have solved them”. This is important as it will make sure the problem level increases gradually. After 20–30 questions the problems tend to become quite tough. Solve 100.
This should be followed by solving problems in Codeforces and/or Codechef. Challenges will take you a long way to solving problems fast.
Once you're confident you should definitely go for ACM ICPC and other competitive programming competitions - they are really a good addition to your resume.
Competitive coding is fun, and helps you prepare for your interviews too. Make sure you start doing it as early as possible.
Related questions
What makes a problem a good programming problem in competitive programming?
Are there any differences between individual and team based competition approaches in competitive programming?
How can I identify the 16 types of competitive programming questions and how should I approach them?
Where should I ask questions related to competitive programming, like the various sample inputs for a particular problem, etc.?
How do I understand the long questions in competitive programming?
Aneesh Hiregange
Rating of 2100+ on Codeforces
·
5y
Related
How did you start competitive programming?
I came to know about competitive programming during the end of 11th standard. I think I read about IOI somewhere online and got to know about CP.
I started taking part in contests on codeforces and codechef. I remember being very bad at it. I solved only 2 problems in my first 5 contests on codeforces. After that, I gave up since I also had to prepare for JEE.
I started doing CP again once JEE was over. I started to practise more seriously.
My college did not have anyone who did CP seriously at the time. Most people did only hackerrank, and that too only during the placement season. This was slig
I came to know about competitive programming during the end of 11th standard. I think I read about IOI somewhere online and got to know about CP.
I started taking part in contests on codeforces and codechef. I remember being very bad at it. I solved only 2 problems in my first 5 contests on codeforces. After that, I gave up since I also had to prepare for JEE.
I started doing CP again once JEE was over. I started to practise more seriously.
My college did not have anyone who did CP seriously at the time. Most people did only hackerrank, and that too only during the placement season. This was slightly demotivating because CP is always more fun when you have someone to discuss it with.
By the end of the 1st year of college, I had reached mid-expert(~1750) from newbie(~1100). By this time, a few of my friends were also doing CP, although occasionally.
I kept practising and reached CM soon and M by the end of 3rd year (inflation of ratings helped too :|).
There are so many things I have learnt from CP, so many memories I will cherish forever. It gave me many new friends. It gave me a chance to make up for screwing up JEE. It helped me get a good internship and a good job. It enabled me to make some money. But most importantly, it has taught me to never give up.
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Addy Radwan
Competitive programmer since 2013
·
Author has 505 answers and 2.4M answer views
·
8y
Related
What is the right approach to solve competitive programming practice questions ?
You mean “What is the best way to train” - I will answer this, but try to search with the right form of question for other answers.
I’m now describing what I’m doing nowadays while solving problems offline, this may not be the best thing in the world, but it works good for me, and I believe in that, so I’m sharing it with you.
I pick the problem.
Don’t look at anything except the text of the problem (don’t look at the tags, comments, contest level, problem level).
I think on paper not PC, I visualize the problem using my pencil
If you didn’t got a solution (for maybe few hours of thinking), go see
You mean “What is the best way to train” - I will answer this, but try to search with the right form of question for other answers.
I’m now describing what I’m doing nowadays while solving problems offline, this may not be the best thing in the world, but it works good for me, and I believe in that, so I’m sharing it with you.
I pick the problem.
Don’t look at anything except the text of the problem (don’t look at the tags, comments, contest level, problem level).
I think on paper not PC, I visualize the problem using my pencil
If you didn’t got a solution (for maybe few hours of thinking), go see the tutorial.
If you still don’t have an idea in your mind or a solution, ask a friend who solved the problem for a hint or see some of the accepted solutions, and try to figure out only the whole idea of the solution.
Now you got a solution, even if it’s not yours from the first time, even if you got some help, Write it on paper, I write some sort of pseudo code, but it’s not a real pseudo code, it’s much untidy with only important points and with only English words with some untidy math symbols (mostly it’s only some non uniform symbols, which may have no meaning to anyone else just me) just like this(it was a problem from the last week, on Codeforces, it’s a random paper from my studying papers “IT ALWAYS WHITE PAPERS, AND I RECOMMEND THIS FOR YOU TOO” ):
Go code it, submit and wait for verification.
If the answer is not accepted, don’t look at the test cases, go back to your paper, work again, try to write cases on yourself, catch the problem ans edit your solution and submit again.
If you did the last step for many times, but still don’t get accepted, check the testcases, and try again.
Now I will assume you got accepted, it’s not the end, you didn’t finish yet, go see the tutorial and see your friends solutions and other guys solutions.
Let’s wrap it up:
Hope this help.
Yamini Sharma
Lived in Muscat, Oman
·
Upvoted by
Vishal Chincholi
, B.E Computer Science, JSS Science and Technology University, Mysuru (2021) · Author has 64 answers and 1.5M answer views
·
6y
Related
How did you start competitive programming?
I began competitive coding in December last year. I t has been a great experience till now. At the start, I literally had no knowledge of Data Structures and Algorithms except arrays and loops which are the basic things you need to crack an IT company's job interview.
Firstly, I picked up Python. I had heard a lot about this language being simple because of it's pretty understandable syntax and it's huge application in the popular field of machine learning and artificial intelligence.
In around a month's time I was able to master Python. I actually wanted to learn this language as prerequisite f
I began competitive coding in December last year. I t has been a great experience till now. At the start, I literally had no knowledge of Data Structures and Algorithms except arrays and loops which are the basic things you need to crack an IT company's job interview.
Firstly, I picked up Python. I had heard a lot about this language being simple because of it's pretty understandable syntax and it's huge application in the popular field of machine learning and artificial intelligence.
In around a month's time I was able to master Python. I actually wanted to learn this language as prerequisite for learning machine learning. Well, everything needs practice. I started practicing on various competitive coding websites like Geeks For Geeks, Hackerrank and Hackerearth to name a few.
As I continued practicing a lot of questions, I felt the need to learn more complex data structures like stacks, queues, linked lists and trees as well as various algorithms and programming paradigms like dynamic programming and divide and conquer.
I slowly shifted to C++ as I felt more comfortable with it. It's faster than Python though and is a better language for competitive coding. Learning C++ was a bit easier because I had developed the logic required to solve basic questions using Python. For a beginner I would recommend learning Python first before jumping into C++.
In every site, there are a lot of coding challenges which are really beneficial in improving the coding skills. When you are stuck at some questions, there are a lot of resources in the internet to help you out. I learnt Python and basics of programming on YouTube and till date if I don’t understand some algorithm, I learn about that on YouTube.
Competitive coding has both been a fun as well as source of frustration, but the former is dominant. I would say coding is not just typing out some lines of code, its more than that. Debugging your code is the real deal. If you are an expert at debugging, you are an expert at coding. And to become an expert at debugging, you really need a lot of practice and hardworking.
Hardwork leads to success and I hope one day I become a successful person in the field of computer science/IT.
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There are a lot of AI tools out there right now—so how do you know which ones are actually worth your time? Which tools are built for students and school—not just for clicks or content generation? And more importantly, which ones help you sharpen what you already know instead of just doing the work for you?
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Rohilla
Studied VLSI Design (Graduated 2006)
·
6y
Related
In programming, how are subsets, subarrays, and subsequences different?
Per my understanding, for example, we have a list say [3,5,7,8,9]. here
subset doesn’t need to maintain order and has non-contiguous behavior. For example, [9,3] is a subset
subsequence maintain order and has non-contiguous behavior. For example, [5,8,9] is a subsequence
sub array maintains order and has contiguous behavior. For example, [8,9] is a sub array
Paras Avkirkar
Competitive Programmer, 200+ AC at Codechef+Spoj+Codeforces
·
8y
Related
What are some algorithms and data structures every competitive programmer should know?
Sorting Algorithms:
Basic sorting algorithms like quick sort and merge sort are rarely needed in competitive programming. Because, we always have some or the other optimised library function like
std::sort()
in C++ or other sort in programming languages.
A competitive programmer must know
Bucket sort - Wikipedia
. In most of the highly time-constraint competitive programming problems, where the nature of the input is already mentioned,
like input will only contain k character symbols
, then you can sort the input under
[math]O(n + k)[/math]
using bucket sort, instead of
[math]O(nlg(n))[/math]
using library sort.
2. Sear
A2A.
Sorting Algorithms:
Basic sorting algorithms like quick sort and merge sort are rarely needed in competitive programming. Because, we always have some or the other optimised library function like std::sort() in C++ or other sort in programming languages.
A competitive programmer must know Bucket sort - Wikipedia. In most of the highly time-constraint competitive programming problems, where the nature of the input is already mentioned, like input will only contain k character symbols, then you can sort the input under [math]O(n + k)[/math] using bucket sort, instead of [math]O(nlg(n))[/math] using library sort.
2. Search Algorithms:
In many of the competitive programming problems, you need to search indices of elements and perform some kind of comparison on those indices. Binary search algorithm - Wikipedia comes into play under such scenarios.
There are many other search algorithms like Interpolation search - Wikipedia and Exponential search - Wikipedia but they are in some way bounded to same algorithmic complexity of [math]lg(n)[/math] .
3. Graph Algorithms:
Depth-first search - Wikipedia, Breadth-first search - Wikipedia, Dijkstra's algorithm - Wikipedia for visiting capitals usually mentioned in problem story, Topological sorting - Wikipedia for ordering certain tasks or city to visit, Prim's algorithm - Wikipedia and Kruskal's algorithm - Wikipedia for finding Minimum Spanning Tree, Bellman–Ford algorithm - Wikipedia and Floyd–Warshall algorithm - Wikipedia for finding all pair shortest path.
For problems where you wish to represent a subset of elements in a set with some common label, where you to want perform special operation mentioned in the problem story on a subset, in such cases you will find Disjoint-set data structure - Wikipedia with union-find by rank algorithm as best suited for time constraints.
4. Divide and Conquer Algorithms:
Fast exponentiation algorithm like Modular exponentiation - Wikipedia which uses divide and conquer strategy is very popular. There are many competitive programming number-theory problems which says “modulo the final answer by [math]10^9 + 7[/math]” , almost all such problems involve fast-exponentiation in one way or the other.
Segment tree - Wikipedia based algorithm uses divide and conquer strategy along with memoization to perform Range Based Queries.
5. Greedy Algorithms:
There are frequent Game Theory problems on Competitive Coding platforms, having description like “Player A plays some move, Player B plays some other move, who will win if both play optimally when Player A makes first move”. Under such cases, you need to find some greedy choice in calculating.
There are other problems like you have to reduce some resource-item and maximise some profit-item mentioned in the problem story.
For problems like above, unlike Sorting-Search problems, there is no set of finite number of algorithms made. You have to solve problems having greedy paradigm.
Solve Activity selection problem - Wikipedia, Job Sequencing Problem, you will get the idea.
6. Dynamic Programming Algorithms:
Like Greedy Algorithm Paradigm, DP problems don’t have finite set of algorithms. You have to practice problems with “dp” tag.
Solve Knapsack problem - Wikipedia, Edit distance - Wikipedia, Longest increasing subsequence - Wikipedia, Longest common subsequence problem - Wikipedia, Coin Change, Rod-Cutting problem. This are popular problems under DP paradigm.
For both Greedy and Dynamic algorithms, you need to solve problems and not learn algorithms. After this only, you will get a gist of constructing your own algorithms.
7. String based Algorithms:
Suffix-Array building algorithm, KMP algorithm are very frequent algorithms needed in competitive programming. But many of the time we have library function to do pattern finding like std::string.substring() .
8. Geometry Algorithms:
Segment-Line intersection check algorithm, Convex hull check algorithm, are also popular
9. Bit Algorithms:
Karatsuba algorithm - Wikipedia, Fenwick tree - Wikipedia which uses bitwise indexing
Bullet 4 and 5 are algorithm paradigms, they don’t have any set of algorithms to learn. You need to practice problems of those paradigm.
For data structures:
Binary Search Tree (mostly implemented using array based indexing, I had never seen someone implementing them using pointers, since we have memory constraint at servers at Competitive Coding Platforms)
Heap (maxHeap/minHeap mostly implemented using array based indexing)
Graph
Adjacency matrix (2-dimensional array),
Adjacency list (Use vector if you are using C++, or Vector of Vector if you are using Java).
Trie
Suffix Tree
It is a compressed variant of Trie.
Segment Tree/Fenwick Tree
You will see how they are use for Range Queries. Like return me minimum element between i and j. Or even range-update queries. Add/Subtract value x to each element between i to j, then later return Min/Max element between p to q.
I personally like this answer by Mostafa Saad Ibrahim Mostafa Saad Ibrahim's answer to What are the algorithms required to solve all problems (using C++) in any competitive coding contest?
He summarised everything under single image.
Happy Coding!
Rajandeep Singh
Software Engineer at Paytm (company) (2019–present)
·
5y
Related
In programming, how are subsets, subarrays, and subsequences different?
There are 3 terms subarray,subsequence,subset:-
subarray->ordered according to index and contiguous.
subsequence->ordered according to index and not contiguous.
subset->not ordered and not contiguous.
example arr[]={5,6,7,8}
subarray can be {5,6,7},{6,7,8},{5,6},etc
subsequence can be {5,7,8],{5,6,8},etc
subset can be {6,8,5},{7,5,6},etc.
Nathan Slaughter
Software Developer & Automation Engineer at Banks (2013–present)
·
5y
In many cases the same solution techniques will apply to problems involving anything called a substring, subsequence, or subarray. In fact the concepts overlap a lot and thus in many cases they're amenable to the same types of analysis. But in fact a sequence, array, and string are distinguishable and it can be useful to understand them more precisely.
A sequence is an ordered set of items. The underlying type of the items doesn't matter to it's identity as a sequence. In fact, the items may be of different type (e.g. string and number) and still be a sequence of a more abstract type, which we
In many cases the same solution techniques will apply to problems involving anything called a substring, subsequence, or subarray. In fact the concepts overlap a lot and thus in many cases they're amenable to the same types of analysis. But in fact a sequence, array, and string are distinguishable and it can be useful to understand them more precisely.
A sequence is an ordered set of items. The underlying type of the items doesn't matter to it's identity as a sequence. In fact, the items may be of different type (e.g. string and number) and still be a sequence of a more abstract type, which we are simply calling “item.”
An array refers specifically to contiguous locations in memory. A programmer should expect to access a new item in an array by reading a new space in memory. This enables pointer arithmetic where you can refer to an item in an array by an offset from the array's base location and a width (size) of the items. If we're talking strictly in programming terms then I would object to use of the term “array” to refer to items of different types.
A string is a sequence of characters in an alphabet. The underlying memory is irrelevant. For instance, UTF encodings use different sizes for different characters. Your alphabet could be defined as the symbols of some character encoding (e.g ASCII or UTF-8) or something simpler and adapted to the problem such as a and b. The point is that an alhabet is a defined finite set. And without that I would say you don't have a string, even though you may hear some people refer to something like “a string of real numbers.”
Hopefully from these definitions you can see how the concepts are related and recognize the times when making the distinction will help you to find solutions.
You will need to be especially watchful when your string's character type are not uniform width (e.g. UTF encodings). Then you have to write the algorithms in a way that compares at a higher-level.
Related questions
What is difference between subarray and contiguous subarray?
In programming, how are subsets, subarrays, and subsequences different?
What is the difference between subString() and subSequence()?
What is the difference between a competitive problem and an interview problem in coding?
What is the difference between constructive questions and other questions at Codeforces (programming competitions)?
What makes a problem a good programming problem in competitive programming?
Are there any differences between individual and team based competition approaches in competitive programming?
How can I identify the 16 types of competitive programming questions and how should I approach them?
Where should I ask questions related to competitive programming, like the various sample inputs for a particular problem, etc.?
How do I understand the long questions in competitive programming?
How do I know if an algorithm will pass the time limit in competitive programming questions?
How do you determine which problem is suitable for you at your level in competitive programming?
What is the difference between hacker and cracker?
How is hacking different from competitive programming?
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11372 | http://dynamicmathematicslearning.com/viviani-general.html | 2D Generalizations of Viviani's Theorem
Viviani's Theorem is named after Vincenzo Viviani, a 17th century mathematician, who was a student of Evangelista Torricelli, the inventor of the barometer. The theorem states the surprising result that the sum of the (perpendicular) distances from a point to the sides
of an equilateral triangle is constant. The theorem generalizes to (convex) polygons that are equilateral or equi-angled, or to 2n-gons with opposite sides parallel as shown respectively by the three interactive sketches below.
A free learning activity with a PDF worksheet that guides learners to discover and formulate Viviani's theorem, and to explain why (prove) that it is true, together with the further explorations below, is given in my book Rethinking
Proof with Sketchpad (which is now completely free to download at the preceding link).
"The process of generalization, instead of leading from elements to classes, leads from classes to classes ... we shall regard abstraction as class formation, and generalization as class extension ...." - Zoltan Dienes (1961, pp. 282; 296). On Abstraction and Generalization. Harvard Educational Review, 31(3), pp. 281-301.
Point A Point A Point On Path A Segment Circle Point On Path A Segment Circle Circle Inter section A Segment Segment Point P Line Line Line Line Perpendicular Inter section P Perpendicular Inter section P Segment Segment Perpendicular Inter section P Segment Perpendicular Inter section P Segment Perpendicular Inter section P Segment Segment Segment Segment Point Circle Inter section Point Circle Inter section Point Circle Inter section Point Circle Inter section Point Circle Inter section Pentagon Viviani generalizes to any (convex) equilateral polygon Path Marker Path Marker Drag P to check the sum of distances A 1 A 2 = 6.17 cm A 2 A 3 = 6.17 cm A 3 A 4 = 6.17 cm A 4 A 5 = 6.17 cm A 5 A 1 = 6.17 cm Path Marker Path Marker Path Marker P P 1 = 3.56 cm Segment Inter section Parallel Parallel Inter section Segment Segment Segment Inter section Parallel Parallel Inter section Segment Segment Segment Inter section Parallel Parallel Inter section Segment Segment Segment Inter section Parallel Parallel Inter section Segment Segment Segment Inter section Parallel Parallel Inter section Segment Segment P 2 P = 4.06 cm P 3 P = 4.60 cm P 4 P = 4.91 cm P 5 P = 3.48 cm P P 1 + P 2 P + P 3 P + P 4 P + P 5 P = cm These are the keyboard-only Toolplay instructions 2D Generalizations of Viviani's Theorem
Investigate
1) Drag point P or any of the red vertices to explore the results.
2) Use the LINK buttons in the sketch above to move to a) a hexagon with opposite sides parallel and b) an equi-angular pentagon.
3) Click on the Show Hint button in the equi-angular pentagon page for a hint to constructing a logical
explanation (proof) for the above result, or if you're really stuck, go to my 2005 paper in Mathematics in School at: Crocodiles
and Polygons.
4) Note that the results hold even when P is outside the polygon, or outside a pair of parallel lines, provided we regard distances respectively falling completely outside the polygon or outside the parallel lines as negative; in other words using directed distances (or equivalently, vectors). However, Sketchpad does not measure 'negative' distances, so dragging P outside will appear to no longer give a constant sum.
Further Generalizations with Equi-inclined lines
Viviani's theorem can be even further generalized by constructing lines to the sides of the above sets of polygons so that they form equal angles with the sides as shown with a dynamic sketch at Further generalizations of Viviani's theorem.
The theorem also generalizes to 3D as shown at 3D Generalizations of Viviani's Theorem.
A Variation on Viviani: Clough's Theorem
An interesting variation of Viviani's theorem was experimentally discovered by a Bishops Diocesan College schoolboy, Clough, in 2003 and is available at: Clough's Theorem and some generalizations.
Directed Distances
As mentioned in 4) above, Viviani's theorem and its various generalizations provide a good context for introducing talented students to directed distances when considering the case when the point P moves outside the polygon. For example, read my paper The Value of using Signed Quantities in Geometry in Learning & Teaching Mathematics, Dec 2020.
Back to "Dynamic Geometry Sketches"
Back to "Student Explorations"
Created by Michael de Villiers, 2011; updated 5 May
2013; 14 April 2019; 8 March 2021; 27 Feb 2024. |
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18.03SCF11 text: The Characteristic Polynomial
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The Art of Problem Solving
The Art of Problem Solving Introduction Series (Gr. 6-10)
The Art of Problem Solving Introduction to Counting & Probability
The Art of Problem Solving: Introduction to Counting & Probability Set
The Art of Problem Solving: Introduction to Counting & Probability Set
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Includes the Student Text and Solutions Manual for the Intro to Counting & Probability Level.
Publisher's Description of The Art of Problem Solving: Introduction to Counting & Probability Set
A thorough introduction for students in grades 7-10 to counting and probability topics such as permutations, combinations, Pascal's triangle, geometric probability, basic combinatorial identities, the Binomial Theorem, and more.
Learn the basics of counting and probability from former USA Mathematical Olympiad winner David Patrick. Topics covered in the book include permutations, combinations, Pascal's Triangle, basic combinatorial identities, expected value, fundamentals of probability, geometric probability, the Binomial Theorem, and much more.
The text is structured to inspire the reader to explore and develop new ideas. Each section starts with problems, so the student has a chance to solve them without help before proceeding. The text then includes solutions to these problems, through which counting and probability techniques are taught. Important facts and powerful problem solving approaches are highlighted throughout the text. In addition to the instructional material, the book contains over 400 problems. The solutions manual contains full solutions to all of the problems, not just answers.
This book is ideal for students who have mastered basic algebra, such as solving linear equations. Middle school students preparing for MATHCOUNTS, high school students preparing for the AMC, and other students seeking to master the fundamentals of counting and probability will find this book an instrumental part of their mathematics libraries.
Paperback (2nd edition). Text: 256 pages. Solutions: 120 pages.
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Category Description for The Art of Problem Solving Introduction Series (Gr. 6-10)
This is an outstanding math program for the math-gifted student. It is rigorous and oriented to the independent problem-solver. The texts are based on the premise that students learn math best by solving problems - lots of problems - and preferably difficult problems that they don't already know how to solve. Most sections, therefore, begin by presenting problems and letting students intuit solutions BEFORE explaining ways to solve them. Even if they find ways to answer the problems, they should read the rest of the section to see if their answer is correct and if theirs is the best or most efficient way to solve that type of problem. Textual instruction, then, is given in the context of these problems, explaining how to best approach and solve them.
Throughout the text there are also special, blue-shaded boxes highlighting key concepts, important things to retain (like formulas), warnings for potential problem-solving pitfalls, side notes, and bogus solutions (these demonstrate misapplications). There are exercises at the end of most sections to see if the student can apply what's been learned. Review problems at the end of each chapter test understanding for that chapter. If a student has trouble with these, he should go back and re-read the chapter. Each chapter ends with a set of Challenge Problems that go beyond the learned material. Successful completion of these sets demonstrates a high degree of mastery.
A unique feature in this series is the hints section at the back of the book. These are intended to give a little help to selected problems, usually the very difficult ones (marked with stars). In this way, students can get a little push in the right direction, but still have to figure out the solution for themselves. The solution manuals do contain complete solutions and explanations to all the exercises, review problems and challenge problems. It is best for students not to access these until they have made several attempts to solve the problems first. I particularly like one of the motivating boxes in the text that coaches, "If at first you don't know how to solve a problem, don't just stare at it. Experiment!". That pretty much sums up the philosophy of the course, encouraging children to take chances, become aggressive problem solvers, and attack problems with confidence. I wonder how far some children would go if they were encouraged this way instead of being spoon fed?
Though this course is used in classroom settings, the texts are student-directed, making them perfect for the independent learner or homeschooler. Students should start the introductory sequence with the Prealgebrabook. Afterwards, begin the Introduction to Algebra. Students will be prepared for both the Introduction to Countingand Probability and Introduction to Number Theory courses after completing the first 11 chapters of Algebra. It won't matter whether they do these along with Algebra, put aside Algebra and complete the other two or finish Algebra first and then do them. All of them should be completed prior to the Introduction to Geometry book. If you are coming into this course from another curriculum, you will probably want to take a placement test to decide where to enter this program. Even if your student has finished Algebra 2 elsewhere, you will want to make sure that all of the material from this series has been covered before continuing on to the Intermediate series.
Taken together, these constitute a complete curriculum for outstanding math students in grades 6-10 and one that prepares them for competitions such as MATHCOUNTS and the American Mathematics Competitions. The material is challenging and in-depth; this is not a course for the mathematically faint of heart. If your child loves math, is genuinely math-gifted, or is interested in participating in math competitions, you definitely need to give this one serious consideration.
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| Grades: | 6-10 |
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Wow! Not only do my 6th and 7th grader enjoy these thinking problems, but I do too! It helps to have a basic understanding of algebra first. Its like Beast Academy for big kids.
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11376 | https://en.wikipedia.org/wiki/Perry%27s_Chemical_Engineers%27_Handbook | Perry's Chemical Engineers' Handbook - Wikipedia
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From Wikipedia, the free encyclopedia
1934 reference book for chemical engineering
Perry's Chemical Engineers' Handbook,8th Edition
Author Don W. Green, Marylee Z. Southard (Editors - 9th edition)
Language English
Subject Chemical Engineering
Publisher McGraw-Hill
Publication date 23 September 2018 (9th Edition)
Media type Hardback
Pages 2272 (9th Edition)
ISBN0-07-142294-3
OCLC72470708
Dewey Decimal660 22
LC ClassTP151 .P45 2008
Perry's Chemical Engineers' Handbook (also known as Perry's Handbook, Perry's, or The Chemical Engineer's Bible)] It has been a source of chemical engineering knowledge for chemical engineers, and a wide variety of other engineers and scientists, through eight previous editions spanning more than 80 years.[citation needed_]
Subjects
[edit]
The subjects covered in the book include: physical properties of chemicals and other materials; mathematics; thermodynamics; heat transfer; mass transfer; fluid dynamics; chemical reactors and chemical reaction kinetics; transport and storage of fluid; heat transfer equipment; psychrometry and evaporative cooling; distillation; gas absorption; liquid-liquid extraction; adsorption and ion exchange; gas–solid, liquid–solid and solid–solid operations; biochemical engineering; waste management, materials of construction, process economics and cost estimation; process safety and many others.
History
[edit]
The first edition was edited by John H. Perry who was a PhD physical chemist and chemical engineer for E. I. du Pont de Nemours & Co. W. S. Calcott (ChE) of DuPont was his assistant editor. It was published in 1934. The second edition was published in 1941. The third edition was edited by John H. Perry and published in 1950 The fourth edition was edited by Robert H. Perry, Cecil H. Chilton, and Sidney D. Kirkpatrick and published in 1963. The fifth edition was edited by Robert H. Perry and published in 1973. The sixth edition ("50th Anniversary Edition")[citation needed] was published in 1984 and edited by Robert H. Perry and Donald W. Green. The 1997 seventh edition was edited by Robert H. Perry and Donald W. Green. The 2640 page 2007–2008 eighth edition was edited by Don W. Green and Robert H. Perry. and published October 2007.
All of the editions of Perry's Chemical Engineering Handbooks.
The 2018–2019 ninth edition was edited by Don W. Green and Marylee W. Southard Don Green, the handbook's editor-in-chief, holds a B.S. in petroleum engineering from the University of Tulsa, and M.S. and PhD. Degrees in chemical engineering from the University of Oklahoma. He is Editor of the 6th, 7th and 8th Editions of Perry's. On the other hand, Marylee Southard, the associate editor, holds B.S., M.S. and PhD Degrees in chemical engineering from the University of Kansas. She is new to the publication of Perry's, but has done significant work in inorganic chemicals production including process engineering, design and product development.
See also
[edit]
Chemical engineer
Distillation Design
Process design
Process engineering
Transport Phenomena
Unit operations
Unit Operations of Chemical Engineering
External links
[edit]
A review by NST Engineers
References
[edit]
^"Review of 7th edition". NST Engineers Inc. Retrieved August 25, 2009.
^Biegler, Lorenz T. (2010). Nonlinear programming: concepts, algorithms, and applications to chemical processes. p.15.
^Perry, Robert H.; Green, Don W. (2008). Perry's Chemical Engineers' Handbook, Eighth Edition. ISBN978-0071422949.
^"Perry's Chemical Engineers' Handbook 9th Edition".
^Southard, Marylee Z.; Green, Don W. (August 29, 2018). Perry's Chemical Engineers' Handbook, 9th Edition. ISBN978-0071834087.
^"Perry's Chemical Engineers' Handbook 9th Edition".
Retrieved from "
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Perry's Chemical Engineers' Handbook
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11377 | https://www.quora.com/How-many-amps-does-a-toaster-use | How many amps does a toaster use? - Quora
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How many amps does a toaster use?
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·
1y
Toasters typically use between 800 to 1,500 watts of power, which corresponds to around 3 to 7 amps on a standard 120V household electrical circuit.
Upvote ·
Steven Wilson
MSEE & BSEE, 50+yrs NW R&D EE, Power/Control/Comm Systems · Author has 2.5K answers and 6.7M answer views
·Updated 2y
It depends on the voltage at which the toaster operates, and to some extent on the number of slices the toaster cooks at once. In the US, toasters almost universally operate at 120V. Most toasters designed for 120V circuits use an average of about 1200W, which corresponds to about 10A. This is about 1/2 of the full-load current of a 20A breaker, and 2/3 of the full-load current of a 15A breaker, which is why you want to avoid having (for example) your toaster, your microwave oven and your coffee maker on the same receptacle circuit, let alone on the same circuit as your refrigerator.
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Richard Neal
Former Fleet Mechanic -Explosive Ordnance Tech -Machinist at Lockheed Martin (company) (1986–2016) · Author has 10.1K answers and 12.7M answer views
·6y
Watts divided by Volts = Amps, So I just went out into the kitchen and looked at our little, 2-slice toaster (650W. / 120 Volts. rated) this would draw 5.4 Amps. I would assume that a 4-slice toaster would probably draw twice as much current and a small “toaster oven” would be in the 10–12 Amp range. Most small appliances have a rating label on them (my toaster had it on the underside). These usually dispaly V oltage and W atts, leaving you to calculate the current (A mps.)
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How many amps does an induction cooktop use?
Horacio Perez
Former Principal Engineer (1983–2014) · Author has 183 answers and 174.9K answer views
·6y
It depends on the rated wattage of the toaster, an easy way to calculate the toaster amperage is dividing the the toaster power rating in watts by the rated voltage, look the nameplate, there is a small difference because the real voltage can differ from the rated one, the difference is negligent.
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9 1
David Lewis
lived with people · Author has 8.3K answers and 3.8M answer views
·5y
Current consumption may be noted on the appliances service plate.
If the wattage of the toaster is known. Use ohms law to calculate the current consumption. In North America our line voltage for small appliances is 120 Volts RMS AC.
Alternatively you may plug the toaster into a Kill-A-Watt device and read the numbers as displayed.
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Kenneth Lundgren
, B.S. Electrical Engineering, Illinois Institute of Technology Chicago - Illinois Tech (1963) · Author has 9.8K answers and 12.8M answer views
·7y
Related
A toaster takes 5 amperes from a 230-watt power line. How much power is consumed by the toaster?
A toaster takes 5 amperes from a 230-watt power line. How much power is consumed by the toaster?
One would have to assume you really mean a 230 volt line. So, 230v 5 = 1150 watts.
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Tony Christian Ratcliffe
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·5y
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A typical toaster (110 volts) has a current of 7 amps when toasting. What is the resistance?
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James F
Former Electrician, Studied Electrical Engineering and IT
·1y
Related
How much electricity does a toaster use?
The typical toaster wattage range is 500W-1800W in the US, 1096W is the average based on 226+ popular toasters. UK toaster wattages are typically higher.
Their actual electricity usage will be slightly lower than their listed wattage.
At its peak, my toaster consumed 91.5% of its listed wattage.
It consumed 0.05 kWh, on medium, to toast 2 slices of bread.
Assuming you have a 1000W toaster (running at max / its wattage / power rating) and it takes 3 minutes per use, once per day, you’re looking at 50 Wh consumed per use, 0.350 kWh per week, 1.55 kWh per month, and 18.25 kWh annually.
Hope that helps
Continue Reading
The typical toaster wattage range is 500W-1800W in the US, 1096W is the average based on 226+ popular toasters. UK toaster wattages are typically higher.
Their actual electricity usage will be slightly lower than their listed wattage.
At its peak, my toaster consumed 91.5% of its listed wattage.
It consumed 0.05 kWh, on medium, to toast 2 slices of bread.
Assuming you have a 1000W toaster (running at max / its wattage / power rating) and it takes 3 minutes per use, once per day, you’re looking at 50 Wh consumed per use, 0.350 kWh per week, 1.55 kWh per month, and 18.25 kWh annually.
Hope that helps.
Upvote ·
Chris Mcguire
Approved electrician at InGen (2010–present) · Author has 87 answers and 111.1K answer views
·7y
Related
A toaster takes 5 amperes from a 230-watt power line. How much power is consumed by the toaster?
Power equals voltage multiplied by the current. Power is measured in watts and it would be a 230 volt power line.
So P=VI
P=230x5
P=1150Watts
the power being used would be 1.15kW
Upvote ·
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Charlee Anthony
Personal Finance @ Almedia | Gaming Enthusiast
·Sep 17
What are ways to earn 930 within a month?
I cashed out $1,200 to PayPal in just 30 days - starting with $0 investment. All I did was try out Freecash, and it actually worked.
How I got started
At the start of the year, I set myself a simple challenge: make $930 in one month without picking up another job. I was tired of side hustle lists that required selling stuff, investing money I didn’t have, or waiting months for results.
That’s when I stumbled on a site called Freecash. Signing up took less than a minute, and I even got a $5 bonus just for creating my account. Honestly, I was skeptical - but since it didn’t cost anything, I gave it
Continue Reading
I cashed out $1,200 to PayPal in just 30 days - starting with $0 investment. All I did was try out Freecash, and it actually worked.
How I got started
At the start of the year, I set myself a simple challenge: make $930 in one month without picking up another job. I was tired of side hustle lists that required selling stuff, investing money I didn’t have, or waiting months for results.
That’s when I stumbled on a site called Freecash. Signing up took less than a minute, and I even got a $5 bonus just for creating my account. Honestly, I was skeptical - but since it didn’t cost anything, I gave it a try.
If you want to test something similar, creating an account is simple and low-risk - you could see if it fits your routine too.
What Freecash really is
In plain words, Freecash is a platform that rewards you for completing online offers. Some are quick (like surveys), while others are longer but pay more (like reaching levels in mobile games). The big difference I noticed compared to other apps: everything is upfront. You know exactly what you’ll earn before starting, and cashouts are instant - PayPal, Visa, crypto, or gift cards.
What really convinced me was seeing other users sharing screenshots of cashouts in the community tab. I wasn’t the only one testing it.
If you’re curious, you could just explore Freecash and see what kind of tasks are available.
What you can do on Freecash
Here are the main ways I earned:
Games: I made $65 from one RPG by reaching a certain level. I even spent $10 inside the game to speed up progress, but it was worth it because the payout was much higher.
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Fred Tee
MSEE in Electrical Engineering, University of Southern California (Graduated 1965) · Author has 215 answers and 232.9K answer views
·7y
Related
A toaster takes 5 amperes from a 230-watt power line. How much power is consumed by the toaster?
An idiot must first answer the question correctly.
There is no such thing as a 230 watts power line.
Upvote ·
James F
Former Electrician, Studied Electrical Engineering and IT
·1y
Related
How many watts should a toaster have?
Based on 226+ popular toasters, their listed wattage typically ranges from 500W to 1800W in the US (UK models are slightly higher).
The average in the study came to 1096W.
~19% continued to consume electricity when not in use - less than 1W to just a few watts.
The higher the wattage, the more watts consumed, the quicker the toasting (typically).
So, if you want faster toasting, a higher wattage model should suit you.
The amount of watts a toaster actually consumes will be slightly lower than its listed wattage.
My toaster, at its peak, reached 91.5% of its listed wattage.
Hope that helps.
Upvote ·
9 2
David Wilmshurst
Materials Engineering Mgr - Concrete & Structural Testing · Author has 8.8K answers and 18.5M answer views
·3y
Related
A toaster is connected to a 120-volt supply and its draw 8 amperes. What is the resistance?
A toaster is connected to a 120-volt supply and its draw 8 amperes. What is the resistance?
Answering the question…
A common equation is R = V / I
So, R = 120 V / 8 A = 15 Ω, aka 15 ohms
(Please note my syntax here. Quantities are in italics, and the mandatory space between the number and the unit symbol (r symbol, had I used one). Also that all SI units start with a lower case letter, whereas unit symbols start with lower case letter, unless they are eponymous.)
Discussion.
While it is common to call “R = V / I” or “V = I x R” Ohm’s law, it is also common to do so only when it is applied to a mater
Continue Reading
A toaster is connected to a 120-volt supply and its draw 8 amperes. What is the resistance?
Answering the question…
A common equation is R = V / I
So, R = 120 V / 8 A = 15 Ω, aka 15 ohms
(Please note my syntax here. Quantities are in italics, and the mandatory space between the number and the unit symbol (r symbol, had I used one). Also that all SI units start with a lower case letter, whereas unit symbols start with lower case letter, unless they are eponymous.)
Discussion.
While it is common to call “R = V / I” or “V = I x R” Ohm’s law, it is also common to do so only when it is applied to a material which has a constant(-ish) resistance at all operating points.
Now, many materials, like copper wire, for instance have a measurable coefficient of thermal resistivity. That is, we heat them, and a piece of the material will change resistance. Clearly, if the temperature change is relatively small, the resistance change will be small. And, some materials have a more considerable change of resistivity with temperature. However, for many pure, solid metals, the temperature coefficients are surprisingly similar. From
Table of Resistivity Resistivity and Temperature Coefficient at 20 C Material Resistivity ρ (ohm m) Temperature coefficient α per degree C Conductivity σ x 10 7 /Ωm Ref Silver 1.59 x10 -8 .0038 6.29 3 Copper 1.68 x10 -8 .00386 5.95 3 Copper 1.724 x10 -8 ... ... 4 Copper, annealed 1.72 x10 -8 .00393 5.81 2 Aluminum 2.65 x10 -8 .00429 3.77 1 Tungsten 5.6 x10 -8 .0045 1.79 1 Iron 9.71 x10 -8 .00651 1.03 1 Platinum 10.6 x10 -8 .003927 0.943 1 Manganin 48.2 x10 -8 .000002 0.207 1 Lead 22 x10 -8 ... 0.45 1 Mercury 98 x10 -8 .0009 0.10 1 Nichrome (Ni,Fe,Cr alloy) 100 x10 -8 .0004 0.10 1 Constantan 49 x10 -8 ... 0.20 1 Carbon (graphite) 3-60 x10 -5 -.0005 ... 1 Germanium 1-500 x10 -3 -.05 ... 1 Silicon 0.1-60 ... -.07 ... 1 Glass 1-10000 x10 9 ... ... 1 Quartz (fused) 7.5 x10 17 ... ... 1 Hard rubber 1-100 x10 13 ... ... 1 The resistivity of semiconductors depends strongly on the presence of impurities in the material, a fact which makes them useful in solid state electronics . References: 1. Giancoli, Douglas C., Physics, 4th Ed, Prentice Hall, (1995). 2. CRC Handbook of Chemistry and Physics, 64th ed. 3. Wikipedia , Electrical resistivity and conductivity. 4. Engineering Toolbox Index Tables Reference Giancoli
Now, if we somehow keep the materials at the same temperature, their resistivity will remain as it is at any current / voltage combination. We might then call them “Ohmic”. But, if we allow their temperature to rise, as current rises, then they are strictly non-Ohmic. This is most easily seen in a tungsten light bulb, which has a low off-resistance, and a comparatively high on-resistance.
Regardless, the equation can be used on either Ohmic, or non-Ohmic items. But, many would say that we can only term the equation “Ohm’s law” for the case where the item is Ohmic, whilst still holding that the equation is useful in both cases.
Some of us still would like to have a name for that equation / identity, and for want of a better name, will continue to use the name “Ohm’s law” regardless.
Upvote ·
9 2
James Reizner
Electrical Engineer with over 45 years experience. · Author has 3.2K answers and 12.9M answer views
·3y
Related
A toaster is connected to a 120-volt supply and its draw 8 amperes. What is the resistance?
Do you want to know the hot or cold resistance of the toaster?
Hot Resistance
Let’s start with Ohm’s Law:
R = E/I = 120 volts / 8 amps = 15 Ohms
This is the resistance when the toaster heating element is hot.
[I do believe that perhaps these numbers are made-up, as in the US (I believe this is a question for the US, or at least North America - because of the 120 volts reference) toasters and most other kitchen appliances, per Underwriters Laboratory Standards, are rated in watts - not amps. Not that it really matters - just a comment.]
Cold Resistance
Most toasters use a metal for their heating eleme
Continue Reading
Do you want to know the hot or cold resistance of the toaster?
Hot Resistance
Let’s start with Ohm’s Law:
R = E/I = 120 volts / 8 amps = 15 Ohms
This is the resistance when the toaster heating element is hot.
[I do believe that perhaps these numbers are made-up, as in the US (I believe this is a question for the US, or at least North America - because of the 120 volts reference) toasters and most other kitchen appliances, per Underwriters Laboratory Standards, are rated in watts - not amps. Not that it really matters - just a comment.]
Cold Resistance
Most toasters use a metal for their heating element similar to Nichrome, which increases its resistance as it gets hot (as most metals do).
I did some rough testing with my toaster to determine the ratio of hot to cold resistance (it was about 1.4 times). So with the heating element in the toaster in question cold (at room temperature) I estimate its resistance to be about 11 Ohm’s.
Per Ohm’s Law, at start the toaster would perhaps draw about 11 amps or so, which would drop to 8 amps very quickly (in a second or so).
The actual cold resistance of the toaster in question might be somewhat different than this, but it least gives you some kind of idea.
To determine the actual cold resistance of the toaster in question simply unplug it, connect a multimeter in Ohm’s function to the two metallic ends of the plug, turn the toaster on and read resistance.
Thanks for taking the time to read this!
Upvote ·
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Related questions
How many watts should a toaster have?
How many amps does a 700 watt microwave use?
How many amps are needed for a circuit with a toaster oven and a microwave?
How much electricity does a toaster use?
How many amps does an induction cooktop use?
How many amps does my microwave oven draw?
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Ampere's Law Explained
By R.W. Hurst, Editor
Ampere’s Law describes the relationship between magnetic fields and electric currents, a fundamental concept in electromagnetism. It explains how current produces a magnetic force, guiding the design of circuits, solenoids, coils, and transformers in electrical engineering.
What is Ampere’s Law?
Ampere's Law is a fundamental principle in electromagnetism that describes the relationship between electric current and the resulting magnetic field.
✅ It states that the magnetic field around a closed path is proportional to the electric current passing through it.
✅ It is a fundamental principle of electromagnetism, linking current and magnetic flux.
✅ Used in analyzing coils, solenoids, transformers, and magnetic circuits.
Named after the French physicist André-Marie Ampère, this powerful principle helps us understand the behaviour of magnetic fields generated by electric currents. It is crucial to develop the numerous technologies we use on a daily basis. Understanding Ampere's Law is easier when explored alongside related concepts in basic electricity, which provide the foundation for electrical theory.
The principle states that the line integral of a magnetic field (B) around a closed loop is equal to the product of the permeability of free space (μ₀) and the net electric current (I) passing through the loop. This can be mathematically represented as:
∮ B⋅dl = μ₀I
Ampere’s Law at a Glance
| Aspect | Explanation | Example / Application |
---
| Definition | Magnetic field around a closed loop is proportional to the net electric current passing through it. | Helps calculate fields in wires, coils, solenoids. |
| Formula | ∮ B · dl = μ₀I (line integral of magnetic field equals permeability × current). | Used in physics and engineering calculations. |
| Relation to Biot-Savart Law | Both describe magnetic fields from current. Biot-Savart handles complex geometries; Ampere’s Law suits symmetrical setups. | Magnetic field around a straight wire vs. irregular current paths. |
| Relation to Faraday’s Law | Ampere’s Law: current → magnetic field. Faraday’s Law: changing magnetic field → induced EMF. | Motors, generators, induction coils. |
| Role in Maxwell’s Equations | One of the four fundamental equations of electromagnetism. | Describes interaction of electric and magnetic fields. |
| Key Devices | Guides design of solenoids, transformers, inductors, motors, and generators. | Power systems, telecommunications, energy conversion. |
| Real-World Impact | Essential to modern technology relying on electromagnetism. | Smartphones, computers, power grids, antennas. |
Ampere’s Law and Magnetism
The principle can be applied to determine the magnetic field around current-carrying wires and other conductive materials, as well as within various electrical systems. It is an essential part of Maxwell's equations, a set of four equations that serve as the foundation of classical electromagnetism. These equations relate electric and magnetic fields to their sources (electric charges and currents) and describe how they propagate through space. The connection between electricity and magnetism is central to electromagnetism, where Ampere’s Law works hand-in-hand with Faraday’s Law to explain induction.
It calculates magnetic fields through the Biot-Savart Law, a mathematical expression that relates the magnetic field produced by a steady electric current to the current's geometry. Both principles have specific applications, with the Biot-Savart Law being more suitable for cases with intricate current configurations. At the same time, it is typically employed when dealing with symmetrical setups.
Ampere’s Law has numerous real-life applications, especially in developing and understanding devices and systems that involve electromagnetism. For example, it is used in the design of transformers, inductors, and solenoids, as well as in various applications such as telecommunications systems, motors, and generators. By applying it, engineers can predict and control the magnetic fields generated in these devices, ensuring they function optimally and efficiently.
Gauss’ Law and Electric Fields Around a Circle of Radius
When studying electromagnetism, a common problem is analyzing the behavior of electric fields around a symmetric object, such as a circle of radius r or a sphere. Gauss’ Law is especially powerful in such cases, because it states that the electric flux through a closed surface is proportional to the net charge enclosed. This means the distribution of field lines can be calculated without solving complex integrals directly.
For a uniformly charged circle of radius r, the electric field at a point along the axis can be derived by considering the superposition of contributions from each charge element. The result reveals that the electric field depends on both the radius of the circle and the distance from the observation point. This demonstrates how Gauss’ Law simplifies problems with high symmetry.
Mathematically, the relationship is expressed as:
∮ E · dA = Q / ε₀
Here, E represents the vector field of the electric field, dA is the infinitesimal area vector on the closed surface, Q is the enclosed charge, and ε₀ is the permittivity of free space. By applying this principle, one can determine that electric fields radiate symmetrically outward from charges, with strength diminishing with distance according to the geometry of the surface considered.
The application of Gauss’ Law in analyzing a circle of radius r is connected to Ampere’s Law, as both emphasize symmetry and integration around closed paths. Where Ampere’s Law links magnetic fields to current, Gauss’ Law links electric fields to charge, and together they form part of Maxwell’s equations, the foundation of electromagnetism.
Relationship between Ampere's Law and Faraday's Law
The relationship between Ampere's Law and Faraday's Law of electromagnetic induction is apparent in the phenomenon of electromagnetic induction itself. When a changing magnetic field induces an electric current in a conductive material, the resulting magnetic field generated by this electric current, in turn, affects the overall magnetic field. It helps us understand how these interacting magnetic fields behave and influence each other.
Ampere's Law and its applications in various devices and systems enable numerous technological advancements. For instance, when designing motors and generators, engineers can utilize the principle to optimize the magnetic field within the device, resulting in higher efficiency and improved performance. Ampere’s Law is also linked to the behavior of capacitance and inductance, both of which are essential in circuits and energy storage systems.
In the telecommunications realm, it helps explain the propagation of electromagnetic waves in cables and antennas. It enables engineers to design systems that minimize signal loss and maximize data transfer rates, ensuring that our smartphones, computers, and other devices remain connected and up-to-date.
By understanding the magnetic field lines and the interaction between electric current and magnetic fields, Ampere's Law opens doors to scientific discovery and innovation in numerous fields. From determining the magnetic field at a distance to the thumb rule and hand rule applications, this fundamental principle plays a crucial role in shaping the world of electromagnetism and the technology that surrounds us.
Electromagnetism
It is a cornerstone of electromagnetism that helps us understand the relationship between electric current and how it creates a magnetic field. It is a vital component of Maxwell's equations and intricately connected to other principles, such as Faraday's Law and Biot-Savart's Law. Ampere's Law has numerous applications in real-life scenarios and is essential for the functioning of many devices and systems that rely on electromagnetism. Its significance in the development of technology cannot be overstated, as it continues to drive scientific discovery and innovation. For students exploring fundamentals, the history of concepts like what is electricity and its evolution in electricity history provides valuable context to Ampere’s discoveries.
How does Ampere’s Law relate to Faraday's Law and Biot-Savart Law?
They are all essential principles in electromagnetism that describe various aspects of the interaction between electric currents and magnetic fields. Although each addresses different aspects, these are interrelated, forming a more comprehensive understanding of electromagnetism.
It describes the relationship between an electric current and its generated magnetic field. Mathematically, it states that the line integral of the magnetic field (B) around a closed loop is proportional to the net electric current (I) passing through the loop:
∮ B⋅dl = μ₀I
Ampere’s Law is useful for calculating magnetic fields in highly symmetrical situations, such as around straight wires, loops, or solenoids.
Faraday's Law: Faraday's Law of Electromagnetic Induction describes how a changing magnetic field induces an electromotive force (EMF) in a conductor. Mathematically, it states that the induced EMF is proportional to the rate of change of the magnetic flux (ΦB) through a closed loop formed by the conductor:
EMF = -dΦB/dt
Faraday's Law is fundamental to understanding the operation of devices such as generators, transformers, and induction motors, which rely on converting mechanical and electrical energy.
The Biot-Savart Law calculates the magnetic field at any point in space due to a specific current distribution. Mathematically, it can be expressed as:
dB = (μ₀ / 4π) (Idl × r̂) / r²
The Biot-Savart Law is particularly useful for calculating magnetic fields in complex current configurations without symmetry.
Ampere's Law and Biot-Savart Law
Ampere's Law and Biot-Savart Law: Both deal with the magnetic field generated by an electric current. While the first is useful for calculating magnetic fields in symmetric situations, the Biot-Savart Law applies to a wider range of configurations, including those with intricate geometries. It can be derived from the Biot-Savart Law for specific symmetric situations.
Ampere's Law and Faraday's Law
Ampere's Law and Faraday's Law: These laws are related through Maxwell's equations, which connect electric and magnetic fields. While the first deals with the magnetic field generated by a steady electric current, Faraday's Law deals with the induced EMF resulting from a changing magnetic field. Both laws contribute to our understanding of electromagnetic phenomena and play a role in operating devices that rely on electromagnetism.
The Biot-Savart Law enables us to determine the magnetic field generated by a specific current distribution. Faraday's Law describes how a changing magnetic field can induce an EMF. In cases where the magnetic field changes due to a varying current, the Biot-Savart Law can be used to calculate the magnetic field, and then Faraday's Law can be applied to determine the induced EMF.
All three are interconnected principles in electromagnetism, each addressing a specific aspect of the interaction between the electric current and the electric field. Together, these form a more comprehensive understanding of electromagnetic phenomena and provide a basis for analyzing and designing various devices and systems that rely on electromagnetism.
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11379 | https://www.whitman.edu/mathematics/calculus_online/section17.02.html | sinx
sinx
A simple, but important and useful, type of separable equation is the
first order homogeneous linear equation:
Definition 17.2.1 A first order homogeneous linear differential equation
is one of
the form ˙y+p(t)y=0y˙+p(t)y=0
or equivalently
˙y=−p(t)yy˙=−p(t)y.
◻□
"Linear'' in this definition indicates that both ˙yy˙ and yy
occur to the first power; "homogeneous'' refers to the zero on the
right hand side of the first form of the equation.
Example 17.2.2 The equation ˙y=2t(25−y)y˙=2t(25−y) can be written
˙y+2ty=50ty˙+2ty=50t. This is linear, but not homogeneous. The
equation ˙y=kyy˙=ky, or ˙y−ky=0y˙−ky=0 is linear and
homogeneous, with a particularly simple p(t)=−kp(t)=−k.
◻□
Because first order homogeneous linear equations are separable, we can
solve them in the usual way:
˙y=−p(t)y∫1ydy=∫−p(t)dtln|y|=P(t)+Cy=±eP(t)+Cy=AeP(t),
y˙∫1ydy=∫−p(t)dtln|y|yy=−p(t)y=P(t)+C=±eP(t)+C=AeP(t),
where P(t)P(t) is an anti-derivative of −p(t)−p(t). As in previous
examples, if we allow A=0A=0 we get the constant solution y=0y=0.
Example 17.2.3 Solve the initial value problems ˙y+ycost=0y˙+ycost=0,
y(0)=1/2y(0)=1/2 and y(2)=1/2y(2)=1/2. We start with
P(t)=∫−costdt=−sint,
P(t)=∫−costdt=−sint,
so the general solution to the differential equation is
y=Ae−sint.
y=Ae−sint.
To compute AA we substitute:
12=Ae−sin0=A,
12=Ae−sin0=A,
so the solutions is
y=12e−sint.
y=12e−sint.
For the second problem,
12=Ae−sin2A=12esin2
12A=Ae−sin2=12esin2
so the solution is
y=12esin2e−sint.
y=12esin2e−sint.
◻□
Example 17.2.4 Solve the initial value problem t˙y+3y=0ty˙+3y=0, y(1)=2y(1)=2,
assuming t>0t>0. We
write the equation in standard form: ˙y+3y/t=0y˙+3y/t=0. Then
P(t)=∫−3tdt=−3lnt
P(t)=∫−3tdt=−3lnt
and
y=Ae−3lnt=At−3.
y=Ae−3lnt=At−3.
Substituting to find AA:
2=A(1)−3=A2=A(1)−3=A, so the solution is y=2t−3y=2t−3.
◻□
Exercises 17.2
Find the general solution of each equation in 1–4.
Ex 17.2.1
˙y+5y=0y˙+5y=0
(answer)
Ex 17.2.2
˙y−2y=0y˙−2y=0
(answer)
Ex 17.2.3
˙y+y1+t2=0y˙+y1+t2=0
(answer)
Ex 17.2.4
˙y+t2y=0y˙+t2y=0
(answer)
In 5–14, solve the initial value problem.
Ex 17.2.5
˙y+y=0y˙+y=0, y(0)=4y(0)=4
(answer)
Ex 17.2.6
˙y−3y=0y˙−3y=0, y(1)=−2y(1)=−2
(answer)
Ex 17.2.7
˙y+ysint=0y˙+ysint=0, y(π)=1y(π)=1
(answer)
Ex 17.2.8
˙y+yet=0y˙+yet=0, y(0)=ey(0)=e
(answer)
Ex 17.2.9
˙y+y√1+t4=0y˙+y1+t4−−−−−√=0, y(0)=0y(0)=0
(answer)
Ex 17.2.10
˙y+ycos(et)=0y˙+ycos(et)=0, y(0)=0y(0)=0
(answer)
Ex 17.2.11
t˙y−2y=0ty˙−2y=0, y(1)=4y(1)=4
(answer)
Ex 17.2.12
t2˙y+y=0t2y˙+y=0, y(1)=−2y(1)=−2, t>0t>0
(answer)
Ex 17.2.13
t3˙y=2yt3y˙=2y, y(1)=1y(1)=1, t>0t>0
(answer)
Ex 17.2.14
t3˙y=2yt3y˙=2y, y(1)=0y(1)=0, t>0t>0
(answer)
Ex 17.2.15
A function y(t)y(t) is a solution of ˙y+ky=0y˙+ky=0. Suppose that y(0)=100y(0)=100 and y(2)=4y(2)=4. Find kk and find y(t)y(t).
(answer)
Ex 17.2.16
A function y(t)y(t) is a solution of ˙y+tky=0y˙+tky=0. Suppose that y(0)=1y(0)=1 and y(1)=e−13y(1)=e−13. Find k and find
y(t).
(answer)
Ex 17.2.17
A bacterial culture grows at a rate proportional to its
population. If the population is one million at t=0 and 1.5
million at t=1 hour, find the population as a function of time.
(answer)
Ex 17.2.18
A radioactive element decays with a half-life of 6 years. If
a block of the element has mass 10 kilograms at t=0, find the amount of
the element at time t.
(answer) |
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Discover how ecosystems come in all shapes and sizes, from massive mountain ranges to the creek in your own backyard. In our first segment of Let's Go Enviro, we hear from watershed specialist Michael Kahle, who explains the cycle of matter, water pollution in our community, and how each ecosystem interacts with our planet at large.
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Let’s Go Enviro is a digital video series that teaches environmental science through phenomena, project-based learning, and Georgia’s diverse ecosystems. The video library consists of six units. Units 1-5 include videos that invite students to become environmental stewards in their own communities, while Unit 6 introduces students to a wide range of careers in the industry. All videos are aligned to the Georgia Standards of Excellence for high school environmental science.
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Ecosystems are dynamic in nature; their characteristics can vary over time. Disruptions to any physical or biological component of an ecosystem can lead to shifts in all its populations. All “MS-LS2.C.1” resources
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A complex set of interactions within an ecosystem can keep its numbers and types of organisms relatively constant over long periods of time under stable conditions. If a modest biological or physical disturbance to an ecosystem occurs, it may return to its more or less original status (i.e., the ecosystem is resilient), as opposed to becoming a very different ecosystem. Extreme fluctuations in conditions or the size of any population, however, can challenge the functioning of ecosystems in terms of resources and habitat availability. All “HS-LS2.C.1” resources
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By the end of the eighth grade students should know that: All organisms, both land-based and aquatic, are interconnected by their need for food. This network of interconnections is referred to as a food web. The entire earth can be considered a single global food web, and food webs can also be described for a particular environment. At the base of any food web are organisms that make their own food, followed by the animals that eat them, then the animals that eat those animals, and so forth. All “5D/M4” resources
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11381 | https://math.mit.edu/~roed/courses/211/lectures/Sep-18.pdf | Vectors The Matrix-Vector Product The Dot Product Vectors The Matrix-Vector Product The Dot Product Linear Methods (Math 211) - Lecture 5, §2.2 (with slides adapted from K. Seyffarth) David Roe September 18, 2013 Vectors The Matrix-Vector Product The Dot Product Recall 1 Matrices 2 Matrix Addition and Scalar Multiplication 3 Transposition and Symmetric Matrices 4 Examples Vectors The Matrix-Vector Product The Dot Product Today 1 Vectors 2 The Matrix-Vector Product 3 The Dot Product Vectors The Matrix-Vector Product The Dot Product Example The linear system x1 + x2 − x3 + 3x4 = 2 −x1 + 4x2 + 5x3 − 2x4 = 1 x1 + 6x2 + 3x3 + 4x4 = −1 has coefficient matrix A and constant matrix B, where A = 1 1 −1 3 −1 4 5 −2 1 6 3 4 and B = 2 1 −1 .
Using (matrix) addition and scalar multiplication, we can rewrite this system as 1 −1 1 x1 + 1 4 6 x2 + −1 5 −2 x3 + 3 −2 4 x4 = 2 1 −1 Vectors The Matrix-Vector Product The Dot Product Example The linear system x1 + x2 − x3 + 3x4 = 2 −x1 + 4x2 + 5x3 − 2x4 = 1 x1 + 6x2 + 3x3 + 4x4 = −1 has coefficient matrix A and constant matrix B, where A = 1 1 −1 3 −1 4 5 −2 1 6 3 4 and B = 2 1 −1 .
Using (matrix) addition and scalar multiplication, we can rewrite this system as 1 −1 1 x1 + 1 4 6 x2 + −1 5 −2 x3 + 3 −2 4 x4 = 2 1 −1 Vectors The Matrix-Vector Product The Dot Product This example illustrates the fact that solving a system of linear equations is equivalent to finding the coefficients of a linear combination of the columns of the coefficient matrix A so that the result is equal to the constant matrix B.
Vectors The Matrix-Vector Product The Dot Product Notation and Terminology R: the set of real numbers.
Rn: set of columns (with entries from R) having n rows.
1 −1 0 3 ∈R4, −6 5 ∈R2, 2 3 −7 ∈R3.
The columns of Rn are also called vectors or n-vectors.
To save space, a vector is sometimes written as the transpose of a row matrix.
1 −1 0 3 T ∈R4 Vectors The Matrix-Vector Product The Dot Product The Matrix-Vector Product Let A = a1 a2 · · · an be an m × n matrix with columns a1, a2, . . . , an, and x = x1 x2 . . .
xn T any n-vector.
The product Ax is defined as the m-vector given by a1x1 + a2x2 + · · · anxn, i.e., Ax is a linear combination of the columns of A (and the coefficients are the entries of x, in order).
As with matrix addition, there is a constraint on the size of the inputs: the number of columns of A must equal the number of rows of x.
Vectors The Matrix-Vector Product The Dot Product Matrix Equations If a system of m linear equations in n variables has the m × n matrix A as its coefficient matrix, the n-vector b as its constant matrix, and the n-vector x as the matrix of variables, then the system can be written as the matrix equation Ax = b.
Vectors The Matrix-Vector Product The Dot Product Theorem (§2.2 Theorem 1) Every system of linear equations has the form Ax = b where A is the coefficient matrix, x is the matrix of variables, and b is the constant matrix.
Ax = b is consistent if and only if b is a linear combination of the columns of A.
If A = a1 a2 . . .
an , then x = x1 x2 . . .
xn T is a solution to Ax = b if and only if x1, x2, . . . , xn are a solution to the vector equation a1x1 + a2x2 + · · · anxn = b.
Vectors The Matrix-Vector Product The Dot Product Example Let A = 1 0 2 −1 2 −1 0 1 3 1 3 1 and y = 2 −1 1 4 1 Compute Ay.
2 Can b = 1 1 1 be expressed as a linear combination of the columns of A? If so, find a linear combination that does so.
Vectors The Matrix-Vector Product The Dot Product Example (continued) 1 Ay = 2 1 2 3 + (−1) 0 −1 1 + 1 2 0 3 + 4 −1 1 1 = 0 9 12 2 Solve the system Ax = b for x = x1 x2 x3 x4 T. To do this, put the augmented matrix A b in reduced row-echelon form.
1 0 2 −1 1 2 −1 0 1 1 3 1 3 1 1 →· · · → 1 0 0 1 1 7 0 1 0 1 −5 7 0 0 1 −1 3 7 Since there are infinitely many solutions, simply choose a value for x4. Taking x4 = 0 gives us 1 1 1 = 1 7 1 2 3 −5 7 0 −1 1 + 3 7 2 0 3 .
Vectors The Matrix-Vector Product The Dot Product Example (continued) 1 Ay = 2 1 2 3 + (−1) 0 −1 1 + 1 2 0 3 + 4 −1 1 1 = 0 9 12 2 Solve the system Ax = b for x = x1 x2 x3 x4 T. To do this, put the augmented matrix A b in reduced row-echelon form.
1 0 2 −1 1 2 −1 0 1 1 3 1 3 1 1 →· · · → 1 0 0 1 1 7 0 1 0 1 −5 7 0 0 1 −1 3 7 Since there are infinitely many solutions, simply choose a value for x4. Taking x4 = 0 gives us 1 1 1 = 1 7 1 2 3 −5 7 0 −1 1 + 3 7 2 0 3 .
Vectors The Matrix-Vector Product The Dot Product Example (continued) 1 Ay = 2 1 2 3 + (−1) 0 −1 1 + 1 2 0 3 + 4 −1 1 1 = 0 9 12 2 Solve the system Ax = b for x = x1 x2 x3 x4 T. To do this, put the augmented matrix A b in reduced row-echelon form.
1 0 2 −1 1 2 −1 0 1 1 3 1 3 1 1 →· · · → 1 0 0 1 1 7 0 1 0 1 −5 7 0 0 1 −1 3 7 Since there are infinitely many solutions, simply choose a value for x4. Taking x4 = 0 gives us 1 1 1 = 1 7 1 2 3 −5 7 0 −1 1 + 3 7 2 0 3 .
Vectors The Matrix-Vector Product The Dot Product Example (Example 5, p. 44.) Write 0 for the m-vector of all zeros.
If A is the m × n matrix of all zeros, then Ax = 0 for any n-vector x.
If x is the n-vector of zeros, then Ax = 0 for any m × n matrix A.
As with matrices, we will generally use the symbol 0 to refer to a zero vector of any size.
Vectors The Matrix-Vector Product The Dot Product Properties of Matrix-Vector Multiplication Theorem (§2.2 Theorem 2) Let A and B be m × n matrices, x, y ∈Rn be n-vectors, and k ∈R be a scalar.
1 A(x + y) = Ax + Ay 2 A(kx) = k(Ax) = (kA)x 3 (A + B)x = Ax + Bx Vectors The Matrix-Vector Product The Dot Product The Dot Product The dot product of two n-tuples (a1, a2, . . . , an) and (b1, b2, . . . , bn) is the number (scalar) a1b1 + a2b2 + · · · + anbn.
Theorem (§2.2 Theorem 4) Suppose that A is an m × n matrix and that x is an n-vector. Then the ith entry of Ax is the dot product of the ith row of A with x.
Vectors The Matrix-Vector Product The Dot Product The Dot Product The dot product of two n-tuples (a1, a2, . . . , an) and (b1, b2, . . . , bn) is the number (scalar) a1b1 + a2b2 + · · · + anbn.
Theorem (§2.2 Theorem 4) Suppose that A is an m × n matrix and that x is an n-vector. Then the ith entry of Ax is the dot product of the ith row of A with x.
Vectors The Matrix-Vector Product The Dot Product Example Compute the product 1 0 2 −1 2 −1 0 1 3 1 3 1 2 −1 1 4 = 0 9 12 using dot products.
1 0 2 −1 · 2 −1 1 4 = 0 2 −1 0 1 · 2 −1 1 4 = 9 3 1 3 1 · 2 −1 1 4 = 12 Vectors The Matrix-Vector Product The Dot Product Example Compute the product 1 0 2 −1 2 −1 0 1 3 1 3 1 2 −1 1 4 = 0 9 12 using dot products.
1 0 2 −1 · 2 −1 1 4 = 0 2 −1 0 1 · 2 −1 1 4 = 9 3 1 3 1 · 2 −1 1 4 = 12 Vectors The Matrix-Vector Product The Dot Product The n × n identity matrix, denoted In is the matrix having ones on its main diagonal and zeros elsewhere, and is defined for all n ≥2.
Example 11 (p. 49) shows that for any n-vector x, Inx = x.
For each j, 1 ≤j ≤n, we denote by ej the jth column of In.
Theorem (§2.2 Theorem 5) Let A and B be m × n matrices. If Ax = Bx for every x ∈Rn, then A = B.
Proof.
Aej = Bej so the columns of A and B are the same.
Vectors The Matrix-Vector Product The Dot Product The n × n identity matrix, denoted In is the matrix having ones on its main diagonal and zeros elsewhere, and is defined for all n ≥2.
Example 11 (p. 49) shows that for any n-vector x, Inx = x.
For each j, 1 ≤j ≤n, we denote by ej the jth column of In.
Theorem (§2.2 Theorem 5) Let A and B be m × n matrices. If Ax = Bx for every x ∈Rn, then A = B.
Proof.
Aej = Bej so the columns of A and B are the same.
Vectors The Matrix-Vector Product The Dot Product The n × n identity matrix, denoted In is the matrix having ones on its main diagonal and zeros elsewhere, and is defined for all n ≥2.
Example 11 (p. 49) shows that for any n-vector x, Inx = x.
For each j, 1 ≤j ≤n, we denote by ej the jth column of In.
Theorem (§2.2 Theorem 5) Let A and B be m × n matrices. If Ax = Bx for every x ∈Rn, then A = B.
Proof.
Aej = Bej so the columns of A and B are the same.
Vectors The Matrix-Vector Product The Dot Product Problem Find examples of matrices A and B, and a vector x ̸= 0, so that Ax = Bx but A ̸= B.
Vectors The Matrix-Vector Product The Dot Product Summary 1 Vectors 2 The Matrix-Vector Product 3 The Dot Product |
11382 | https://www.youtube.com/watch?v=g9I6_AZTjQw | co-finite topology // co-finite topology for bsc MSc mathematics // co-finite topology with examples
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in this leacture you will learn about the concept of cofinite topology with example.
topology #topologicalspace #topologies
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Transcript:
बिस्मिल्लाह रहमान रहीम अस्सलाम वालेकुम स्टूडेंट्स तो आज हम देखेंगे की फाइनल टोपोलॉजी किसको बोलते हैं ठीक है फ्रेंड्स तो सबसे पहले हम khoobfanite टोपोलॉजी डेफिनेशन रीड करेंगे दें उसके बाद हम इसको एग्जांपल के थ्रू समझेंगे की cofinate टोपोलॉजी बेसिकली हम किसको बोलते हैं तो देखिए इसकी डेफिनेशन से स्टार्ट करते हैं की कॉफ टोपोलॉजी की डेफिनेशन क्या है आपके पास लेट एक्स बी आर नॉन एम्टी सेट एक्स हमारे पास क्या है कोई सेट है कलेक्शन ऑफ एम्टी सेट एंड ऑल सबसेट टाइम हमारे पास कौन-कौन से एलिमेंट्स होंगे कलेक्शन होगा ता हमारे पास एक एम्टी सेट का mplement इसे फाइन टोपोलॉजी डेफिनेशन होगा एक्स खुद होगा और वह है इस कार्ड को फिनिटी टोपोलॉजी बोलते हैं अब देखिए इसको हम सबसे पहले तो यह देखें तो फाइनल अपॉलिजी आपके पास ही डेफिनेशन फॉर्म लिखते हैं ठीक है तो देखिए सबसे पहले हम क्या करते हैं हमारे पास इसमें क्या होगा एक एम्टी सेट होगा [संगीत] यह आपके पास को फिनिटी टोपोलॉजी की मैथमेटिक्स फॉर्म आती है ठीक है अब देखिए इसके ऊपर हम डेफिनेशन करते हैं की एग्जांपल करते हैं इस डेफिनेशन को समझने के लिए देखिए मैंने क्या बोला की हमारे पास एक्स कोई भी एक सेट है तो एग्जांपल के तौर पर हम यहां पर क्या कर लेते हैं कोई नॉन एम्टी सेट ठीक तो मैंने क्या किया एक्स ले लिया इसमें कोई भी तीन हम एलिमेंट्स ले लेते हैं 1 2 एंड 3 यह वापस नमकीन टेक्नोलॉजी दूसरा सेट एक्स कंप्लीट होना चाहिए और इसके बाद इसमें वह सारे सेट्स हमने लिखने हैं जो की इस एक्स के सबसेट है देखिए सबसे पहले तो एक्स की जो सबसेट बनते एक वैन बनता है दें आपके पास तू बनता है दें इसके बाद नेक्स्ट क्या आता है थ्री आता है इसके अलावा कौन-कौन से सब्जेक्ट्स हैं इसके वह सारे अपने लिखने जैसे की वैन तू हो गया यह भी हमारे पास इसका सबसे है ठीक है दें 13 हमारे पास इसका सबसे आता है और लास्ट में हमारे पास तू थ्री यह में से कोई एक सेटल जिसका सब सेट है एक्स का उसका एक्स के साथ कंप्लीमेंट ले तू अगेन स्टार में होना चाहिए ठीक है देखिए फॉर एग्जांपल मैं क्या करता हूं की यहां से कोई भी तू को ले लेता हूं तो इसको हम क्या करते हैं कंपलीमेंट लेते अगर तू का कंप्लीमेंट ले हम तो इसका मतलब क्या है एक्स में वैन और थ्री है तो वैन और थ्री अगर आप कोई दूसरा एलिमेंट ले और उसका कंप्लीमेंट करें एक्स से अगर मैं यहां पर लेता हूं वैन और तू और इसका मैं क्या करता हूं कंप्लीमेंट करता हूं एक्स के साथ तो एक्स - क्या आएगा वैन तू हमारे पास जो आंसर आएगा इसका क्या आएगा वो सिर्फ आएगा कोई भी सब्जेक्ट ले ता से और उसका आप एक्स के साथ कंप्लीमेंट करें तो आपके पास अगेन जो आंसर आएगा वो आपके पास इस टाइम होना चाहिए तो इसको बोलते की आपकी क्या समझ आई एक्स आपके पास कोई भी सेट होगा तो उसमें से हम ऐसा कलेक्शन लेंगे जिसमें कौन-कौन से मेंबर्स होंगे एक फाइल होगा सेट एक्स कंप्लीट होगा और सारे सेट जिसके आपके पास कंप्लीमेंट हो ठीक है |
11383 | https://math.stackexchange.com/questions/1125013/triangle-in-parabola | geometry - Triangle in parabola - Mathematics Stack Exchange
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Triangle in parabola
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I have a problem. In my triangle one vertex is in the vertex of the parabola and two others are in parabola. This is a isosceles triangle and I know one angle in this triangle : 120 grades. The question is: angle 120 grades must be beside of the vertex of parabola?
Thanks a lot for answer, I am beginner in math.
Which option (1) or (2) is possible?
geometry
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edited Jan 29, 2015 at 15:22
Nelliusz FrącekNelliusz Frącek
asked Jan 29, 2015 at 14:41
Nelliusz FrącekNelliusz Frącek
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Is it given that the equal sides are AB and AC?(If C is the third point in your triangle)Nemo –Nemo 2015-01-29 14:51:53 +00:00 Commented Jan 29, 2015 at 14:51
I updated question.Nelliusz Frącek –Nelliusz Frącek 2015-01-29 15:01:14 +00:00 Commented Jan 29, 2015 at 15:01
If the sum of the three angles in a triangle is 180° and your triangle is isosceles with the equal sides at the vertex, then what other options do you have besides concluding that the 120 ° must be located at the vertex? In other words, I wouldn't mind to see how option 1 would work.imranfat –imranfat 2015-01-29 15:14:10 +00:00 Commented Jan 29, 2015 at 15:14
I upadeted question, sorry for my not very good description. I know that second option is good, but first option (1 - y) is possible in some conditions?Nelliusz Frącek –Nelliusz Frącek 2015-01-29 15:23:26 +00:00 Commented Jan 29, 2015 at 15:23
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If by 120 you mean 120∘120∘ then it must be on the vertex of parabola. Proof is easy. Just take any point A on parabola, which is not vertex (let vertex point be point V) of parabola, then draw line from this point to vertex, then draw line from this point, such that it will form angle with 120∘120∘. You will get point B, which is intersection of new line with other leg of parabola. The two segments AV and AB are not equal, easy to prove.
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answered Jan 29, 2015 at 15:32
Tahir ImanovTahir Imanov
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choose the coordinates so that the equation of the parabola is y=x 2.y=x 2. let the triangle be O A B O A B with O=(0,0),A=(a,a 2),B=(b,b 2)O=(0,0),A=(a,a 2),B=(b,b 2) and ∠A O B=120∘∠A O B=120∘ by cosine rule,
A B 2=O A 2+O B 2+O A∗O B A B 2=O A 2+O B 2+O A∗O B
so that
(a−b)2+(a 2−b 2)2=a 2+a 4+b 2+b 4+(a 2+a 4)(b 2+b 4)−−−−−−−−−−−−−−√(a−b)2+(a 2−b 2)2=a 2+a 4+b 2+b 4+(a 2+a 4)(b 2+b 4)
cleaning it up a bit we end up with
3 a 2 b 2+8 a b−a 2−b 2+3=0 3 a 2 b 2+8 a b−a 2−b 2+3=0
which simplifies to
−2 a b(1+a b)=(a 2+a 4)(b 2+b 4)−−−−−−−−−−−−−−√(1)(1)−2 a b(1+a b)=(a 2+a 4)(b 2+b 4)
from (1)(1) we can see that a a and b b cannot be of the same sign. using symmetry we can assume that a>0,b<0.a>0,b<0.
a special solution is −b=a=1+2–√−−−−−−√−b=a=1+2 to find the general solution we will square (1)(1) and get a quadratic equation for b b
b 2(3 a 2−1)+8 a b+(3−a 2)=0 b 2(3 a 2−1)+8 a b+(3−a 2)=0
and the solution is
b=−2 a±3–√|a 2−1|3 a 2−1 and b<0.b=−2 a±3|a 2−1|3 a 2−1 and b<0.
if you take the negative solution you find that a negative solution exist for 0≤<3–√0≤<3 and for the positive solution you have 1 3–√<a.1 3<a.
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answered Jan 29, 2015 at 16:04
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11384 | https://e.math.cornell.edu/people/belk/measuretheory/StructureOfMeasurableSets.pdf | Structure of Measurable Sets In these notes we discuss the structure of Lebesgue measurable subsets of R from sev-eral different points of view. Along the way, we will see several alternative character-izations of measurability which might help to make the concept seem more intuitive.
We begin by discussing the measures of open sets.
First, recall the following definition.
Definition: Open Set A subset U ⊆R is said to be open if there exists a collection C of open intervals whose union is U.
Note that R is itself open, being the union of the intervals (n−1, n+1) for n ∈Z.
The empty set ∅is also open, being the union of the empty collection of intervals.
The following proposition highlights the important role that open sets play in analysis.
Proposition 1 Continuity Using Open Sets Let f : R →R. Then f is continuous if and only if f −1(U) is open for every open set U ⊆R.
PROOF Suppose first that f −1(U) is open for every open set U ⊆R. Let x ∈R, and let ϵ > 0. Then U = f(x) −ϵ, f(x) + ϵ is open, so f −1(U) is open. Since x ∈f −1(U), there must be an open interval that contains x and is contained in f −1(U). Indeed, there must exist a δ > 0 so that (x −δ, x + δ) ⊆f −1(U). Then |y −x| < δ ⇒ f(x) −f(y) < ϵ for all y ∈R, which proves that f is continuous at x.
Structure of Measurable Sets 2 For the converse, suppose that f is continuous. Let U ⊆R be any open set, and let x ∈f −1(U). Since U is open, there is an open interval containing f(x) that is contained in U. In particular, there exists an ϵ > 0 so that f(x) −ϵ, f(x) + ϵ ⊆U.
But since f is continuous at x, there exists a δ > 0 so that |x −y| < δ ⇒ f(x) −f(y) < ϵ for all y ∈R. It follows that f(y) ∈ f(x) −ϵ, f(x) + ϵ for all y ∈(x −δ, x + δ).
Then (x −δ, x + δ) ⊆f −1(U), which proves that f −1(U) is open.
■ A priori, there is no reason to think that every open set must be measurable, since by the definition an open set might involve an uncountable union of open intervals.
However, the following structure theorem shows that every open set is a countable union of open intervals.
Theorem 2 Structure of Open Sets Every proper open subset of R is a countable, disjoint union of open intervals and open rays.
PROOF Let U be a proper open subset of R. Put an equivalence relation ∼on U by x ∼y if U contains every point between x and y. The equivalence classes under this relation are called the components of U. We claim that each component of U is either an open interval or an open ray.
Let C be a component of U, and let a = inf(U) and b = sup(U), with a = −∞if U has no lower bound and b = ∞if U has no upper bound. If x ∈(a, b), then there must exist points c1, c2 ∈C so that a < c1 < x and x < c2 < b. Since c1 ∼c2 and x lies between c1 and c2, it follows that x ∈C. This proves that (a, b) ⊆C, and we know that C ⊆[a, b]. But if b ∈C, then since b ∈U and U is open there exists an open interval (d, e) ⊆U that contains b. Then it is easy to see that all of (a, b)∪(d, e) must lie in C, a contradiction since e > b. Thus b / ∈C, and similar reasoning shows that a / ∈C, so C = (a, b). Clearly C ̸= R since U is a proper subset of R, so C is either an open interval or an open ray.
Finally, observe that each component of U must contain at least one rational num-ber, and therefore U has only countably many components. Thus U is the countable, disjoint union of its components.
■ Structure of Measurable Sets 3 Corollary 3 Every open subset of R is Lebesgue measurable.
Based on the structure of open sets described in Theorem 2, the measure m(U) of an open set U can be interpreted as simply the sum of the lengths of the components of U. Note, however, that an open set may have infinitely many components, and these may form a fairly complicated structure on the real line. Indeed, the following example illustrates that open sets can behave in very counterintuitive ways.
Proposition 4 Small Open Sets Containing Q For every ϵ > 0, there exists an open set U ⊆R such that m(U) ≤ϵ and U contains the set Q of rational numbers.
PROOF Let ϵ > 0, let q1, q2, . . . be an enumeration of the rational numbers, and let U = [ n∈N qn − ϵ 2n+1, qn + ϵ 2n+1 .
Then U is open, and m(U) ≤ X n∈N m qn − ϵ 2n+1, qn + ϵ 2n+1 = X n∈N ϵ 2n = ϵ.
■ Closed Sets Recall the following definition.
Definition: Closed Set A subset F ⊆R is closed if, for every convergent sequence {xn} of points in F, the point x ∈R that {xn} converges to also lies in F.
That is, a closed set is a set that it closed under the operation of taking limits of sequences. For example, any closed interval [a, b] is closed, since any convergent sequence in [a, b] must converge to a point in [a, b]. The entire real line R is also closed, and technically the empty set ∅is closed as well, since the condition is vacuously satisfied.
Structure of Measurable Sets 4 The following description of closed sets is fundamental.
Proposition 5 Complements of Closed Sets Let F ⊆R. Then F is closed if and only if F c is open.
PROOF Suppose first that F is not closed. Then there exists a sequence {xn} of points in F that converges to a point x ∈F c. Then every open interval (a, b) that contains x must contain a point of the sequence, and therefore no open interval (a, b) that contains x is contained in F c. It follows that F c is not open.
Conversely, suppose that F c is not open. Then there must exist a point x ∈F c that does not lie an any open interval contained in F c. In particular, each of the open intervals (x−1/n, x+1/n) must contain a point xn ∈F. Then the sequence {xn}n∈N in F converges to the point x ∈F c, so F is not closed.
■ Corollary 6 Every closed subset of R is Lebesgue measurable.
We now turn to unions and intersections of open and closed sets. Students of point-set topology will recognize parts (1) and (2) of the following proposition as essentially the definition of a topological space.
Proposition 7 Unions and Intersections of Open and Closed Sets 1.
The union of any collection of open sets in R is open.
2.
The intersection of finitely many open sets in R is open.
3.
The intersection of any collection of closed sets in R is closed.
4.
The union of finitely many closed sets in R is closed.
PROOF For (1), let C be a collection of open sets. For each U ∈C, let IU be a collection of open intervals whose union is U. Then I = S U∈C IU is a collection of open intervals whose union is S C, and therefore S C is open.
Structure of Measurable Sets 5 For (2), it suffices to prove that U ∩V is open if U and V are open. Given such a U and V , let I and J be collections of open intervals whose unions are U and V respectively. Then {I ∩J | I ∈I, J ∈J , and I ∩J ̸= ∅} is a collection of open intervals whose union is U ∩V , and therefore U ∩V is open.
Parts (3) and (4) follow immediately from parts (1) and (2) by taking comple-ments.
■ Though every open set in R is a disjoint union of countably many open intervals, it is not true that every closed set is a disjoint union of closed intervals. Indeed, there exists a very famous closed set called the Cantor set whose structure is much more interesting. To construct the Cantor set, we start with the unit interval: C0 = [0, 1].
Next we remove the middle third of this interval, leaving a union of two closed inter-vals: C1 = h 0, 1 3 i ⊎ h 2 3, 1 i .
Next we remove the middle third of each of these intervals, leaving a union of four closed intervals: C2 = h 0, 1 9 i ⊎ h 2 9, 1 3 i ⊎ h 2 3, 7 9 i ⊎ h 8 9, 1 i .
Proceeding in this fashion, we obtain a nested sequence C0 ⊇C1 ⊇C2 ⊇· · · of closed sets, where Cn is the union of 2n closed intervals, as illustrated in Figure 1. Then the intersection C = \ n∈N Cn is the aforementioned Cantor set.
Figure 1: The first six stages in the construction of the Cantor set.
Structure of Measurable Sets 6 Proposition 8 Properties of the Cantor Set The Cantor set C has the following properties: 1.
C is closed.
2.
C is uncountable. Indeed, |C| = |R|.
3.
m(C) = 0.
PROOF Since C is the intersection of the closed sets Cn, it follows from Propo-sition 7 that C is closed. Furthermore, since Cn is the disjoint union of 2n closed intervals of length 3−n, we know that m(Cn) = 2n3−n = (2/3)n, and it follows that m(C) = inf n∈N m(Cn) = inf n∈N(2/3)n = 0.
Finally, to show that C is uncountable, let {0, 1}∞be the (uncountable) set of all infinite binary sequences, and define a function f : {0, 1}∞→R by f(b1, b2, b3, . . .) = X n∈N 2bn 3n .
It is easy to check that f is injective and the image of f lies in the Cantor set (in fact, f is a bijection from {0, 1}∞to C), and therefore C is uncountable. Indeed, we have |R| = {0, 1}∞ ≤|C| ≤|R| and hence |C| = |R|.
■ Corollary 9 Let M be the collection of all Lebesgue measurable subsets of R. Then |M| = P(R) .
PROOF Clearly |M| ≤ P(R) . But since the Cantor set C has Lebesgue measure zero, every subset of the Cantor set is Lebesgue measurable, i.e. P(C) ⊆M. But since |C| = |R|, it follows that P(C) = P(R) , and hence P(R) ≤|M|.
■ Incidentally, there is some sense in which the structure of the Cantor set is fairly typical for closed sets. In particular, Theorem 2 tells us that any open set can be Structure of Measurable Sets 7 described as the union of a nested sequence U1 ⊆U2 ⊆U3 ⊆· · · where each Un is a finite disjoint union of open intervals and open rays.
Taking complements, we find that any closed set can be described as the intersection of a nested sequence F1 ⊇F2 ⊇F3 ⊇· · · where each Fn is a finite disjoint union of closed intervals and closed rays.
Open Sets and Measurability We are now ready to use open sets and closed sets to give a few alternative descriptions of Lebesgue outer measure and Lebesgue measurability. We begin by describing the Lebesgue outer measure in terms of open sets.
Proposition 10 Open Sets and Outer Measure If S ⊆R, then m∗(S) = inf{m(U) | U is open and S ⊆U}.
PROOF Let x be the value of the infimum. Clearly m∗(S) ≤m(U) for every open set U that contains S, and therefore m∗(S) ≤x. For the opposite inequality, let ϵ > 0, and let C be a cover of S by open intervals so that X I∈C ℓ(I) ≤m∗(S) + ϵ.
Then U = S C is an open set that contains S, so x ≤m(U) ≤ X I∈C m(I) = X I∈C ℓ(I) ≤m∗(S) + ϵ.
Since ϵ was arbitrary, it follows that x ≤m∗(S).
■ We shall now use open sets to give a nice characterization of measurability.
Structure of Measurable Sets 8 Proposition 11 Measurability Using Open Sets Let S ⊆R. Then S is Lebesgue measurable if and only if for every ϵ > 0 there exists an open set U containing S so that m∗(U −S) < ϵ.
PROOF Suppose first that S is measurable, and let ϵ > 0. For each n ∈N, let Sn = S ∩[−n, n], and let Un be an open set containing Sn so that m(Un) < m(Sn) + ϵ 2n.
Let U = S n∈N Un. Then U is an open set containing S and U −S ⊆S n∈N(Un −Sn), so m(U −S) ≤ X n∈N m(Un −Sn) ≤ X n∈N ϵ 2n = ϵ.
For the converse, let S ⊆R, and suppose that for every n ∈N there exists an open set Un containing S so that m∗(Un −S) < 1/n. Let E = T n∈N Un, and note that E is a measurable set containing S. But E −S ⊆Un −S for each n, so m∗(E −S) ≤m∗(Un −S) ≤1 n for each n. We conclude that m∗(E −S) = 0, and therefore E −S is Lebesgue measurable. Then S = E −(E −S) is Lebesgue measurable as well.
■ Corollary 12 Measurability Using Closed Sets Let S ⊆R. Then S is Lebesgue measurable if and only if for every ϵ > 0 there exists a closed set F ⊆S containing S so that m∗(S −F) < ϵ.
PROOF Observe that F is a closed set contained in S if and only if U = F c is an open set containing Sc. Moreover, S −F = U −Sc, so m∗(S −F) < ϵ if and only if m∗(U −Sc) < ϵ, and hence this statement follows directly from applying the previous proposition to Sc.
■ Combining this corollary with the previous proposition yields the following nice result.
Structure of Measurable Sets 9 Corollary 13 Let S ⊆R. Then S is Lebesgue measurable if and only if there exists a closed set F and an open set U so that F ⊆S ⊆U and m(U −F) < ϵ.
Incidentally, there is another function similar to Lebesgue outer measure that is more closely related to closed sets.
Definition: Inner Measure If S ⊆R, the Lebesgue inner measure of S is defined by m∗(S) = sup{m(F) | F is closed and F ⊆S}.
It follows immediately from Corollary 12 that m∗(E) = m(E) for any measurable set E. It is also apparent that m∗(S) ≤m∗(S) for any set S ∈R. The following proposition gives a nice characterization of measurability for sets of finite measure.
Proposition 14 Measurability Using Inner and Outer Measures Let S ⊆R, and suppose that m∗(S) < ∞. Then S is measurable if and only if m∗(S) = m∗(S).
PROOF If S is measurable, then m∗(S) = m(S) = m∗(S). Conversely, suppose that m∗(S) < ∞and m∗(S) = m∗(S). Let ϵ > 0, and let F ⊆S be a closed set and U ⊆R and open set containing S so that m∗(S) ≤m(F) + ϵ 2 and m(U) ≤m∗(S) + ϵ 2.
Then m(U −F) = m(U) −m(F) ≤ m∗(S) + ϵ 2 − m∗(S) −ϵ 2 = ϵ.
Since ϵ was arbitrary, it follows from Corollary 13 that S is measurable.
■ Structure of Measurable Sets 10 Fσ and Gδ Sets As we have seen, every open or closed subset of R is Lebesgue measurable.
The following definition provides many more examples of measurable sets.
Definition: Fσ and Gδ Sets 1. A subset of R is Fσ if it is a countable union of closed sets.
2. A subset of R is Gδ if it is a countable intersection of open sets.
Here F stands for ferm´ e, which is French for “closed”, and σ stands for somme, which is the French word for a union of sets. Similarly, G stands for Gebiet, which is the German word for an open set, and δ stands for Durchschnitt, which is the German word for an intersection of sets.
The following proposition lists some of the basic properties of Fσ or Gδ sets. The proofs are left to the exercises.
Proposition 15 Properties of Fσ and Gδ Sets 1.
An Fσ or Gδ set is measurable.
2.
If S ⊆R, then S has type Fσ if and only if Sc has type Gδ.
3.
Every countable set is Fσ. In particular, the set Q of rational numbers is Fσ, and the set R −Q of irrational numbers is Gδ.
4.
Every open or closed set is both Fσ and Gδ.
The rational numbers provide an example of an Fσ set that is neither open nor closed. Incidentally, it is possible to prove that the rational numbers are not a Gδ set using the Baire category theorem (see §48 of Munkres’ Topology).
Of course, most Fσ sets are not countable. The following example describes an uncountable Fσ set that is neither open nor closed, whose structure is more “typical” for sets of this type.
EXAMPLE 1 Let C ⊆[0, 1] be the Cantor set. Note that any closed interval [a, b] contains a scaled copy of C whose left endpoint is a and whose right endpoint is B.
We now define a sequence F0 ⊆F1 ⊆F2 ⊆· · · of sets as follows: • We start with F0 = C.
Structure of Measurable Sets 11 • Let F1 be the set obtained from C by pasting a scaled copy of C into each interval of [0, 1] −C.
• For each n ≥2, let Fn be the set obtained from Fn−1 by pasting a scaled copy of C into each interval of [0, 1] −Fn−1.
Note that each Fn is a closed set, since the complement F c n is a union of open intervals.
The union F = S n∈N Fn is thus an Fσ set. It is not hard to see that neither F nor F c contains any open intervals, so F is neither open nor closed. Note also that each Fn has measure zero, and therefore F has measure zero.
This set F has a nice description in ternary (base 3). First, observe that the Cantor set C consists of all points x ∈[0, 1] that have a ternary expansion consisting only of 0’s and 2’s, with no 1’s. Then for each n, the set Fn consists of all points x ∈[0, 1] that have a ternary expansion with at most n digits that are 1. For example, the number 475 972 = 0.1110120202020 · · · lies in F4 but not F3. Then the Fσ set F consists of all points x ∈[0, 1] that have a ternary expansion with at most finitely many 1’s.
■ We can reinterpret some of our criteria for measurability involving open and closed sets in terms of Fσ and Gδ sets.
Proposition 16 Measurability Using Fσ and Gδ Sets Let E ⊆R. Then the following are equivalent: 1.
E is Lebesgue measurable.
2.
E = F ∪Z for some Fσ set F and some set Z ⊆R of measure zero.
3.
E = G −Z for some Gδ set G and some set Z ⊆G of measure zero.
PROOF Clearly (2) and (3) both imply (1). For the converse, suppose that E is Lebesgue measurable. For every n ∈N, let Fn be a closed set and Un be an open set so that Fn ⊆E ⊆Un and m(Un −Fn) ≤1/n. Then F = S n∈N Fn is an Fσ set and G = T n∈N Un is a Gδ set such that F ⊆E ⊆G. Moreover, since G −F ⊆Gn −Fn for all n, we know that m(G −F) = 0. Then E = F ∪(E −F) = G −(G −E), where m(E −F) = m(G −E) = 0.
■ Structure of Measurable Sets 12 Borel Sets If X is a set, recall that a σ-algebra on X is any nonempty collection of subsets of X that is closed under taking complements and countable unions. For example, the Lebesgue measurable subsets of R form a σ-algebra on R.
Proposition 17 Intersection of σ-Algebras Let X be a set, and let C be any collection of σ-algebras on X. Then the inter-section T C is also a σ-algebra on X.
PROOF Since ∅∈M for every M ∈C, it follows that ∅∈T C. Next, if S ∈T C, then S ∈M for every M ∈C.
Then Sc ∈M for every M ∈C, and hence Sc ∈T C. Finally, if {Sn} is a sequence in T C, then each M ∈C must contain the entire sequence {Sn}. It follows that S n∈N Sn ∈M for each M ∈C, and hence S n∈N Sn ∈T C.
■ You have probably seen propositions similar to this one in other fields of mathe-matics. For example, a similar fact from group theory is that the intersection of any collection of subgroups of a group G is again a subgroup of G. Similarly, in topology the intersection of any collection of topologies on a set X is again a topology on X.
Definition: Generators for a σ-Algebra Let X be a set, and let C be any collection of subsets of X.
The σ-algebra generated by C is the intersection of all σ-algebras on X that contain C.
It is important for this definition that there is always at least one σ-algebra that contains C, namely the collection P(X) of all subsets of X.
EXAMPLE 2 Let X be a set, and let C be the collection of singleton sets in X, i.e.
C = {x} x ∈X .
Then it is not hard to check that the σ-algebra generated by C consists of all sets S ⊆X for which either S or Sc is countable.
■ Definition: Borel Sets The Borel algebra B is the σ-algebra on R generated by the collection of all open sets. A set B ⊆R is called a Borel set if B ∈B.
Structure of Measurable Sets 13 By definition every open set is a Borel set. Moreover, since the Borel sets are a σ-algebra, the complement of any Borel set is a Borel set, and any countable union of Borel sets is a Borel set.
Proposition 18 Properties of Borel Sets 1.
Every Borel set is measurable.
2.
Every open set, closed set, Fσ set, or Gδ set is a Borel set.
3.
The Borel algebra is generated by the collection of all open intervals.
PROOF For (1), observe that the collection M of all Lebesgue measurable sets is a σ-algebra that contains the open sets. Since B is the intersection of all such σ-algebras, it follows that B ⊆M.
For (2), every open set lies in B by definition. Since B is a σ-algebra, it follows immediately that closed sets, Fσ sets, and Gδ sets lie in B as well.
For (3), let A be the σ-algebra generated by the open intervals. Since B contains the open intervals, we know that A ⊆B. But since every open set is a countable union of open intervals, A contains every open set, and hence B ⊆A.
■ As we will see, open sets, closed sets, Fσ sets, and Gδ sets are among the simplest of the Borel sets. In the rest of this section, we describe the overall structure of the Borel algebra. We will not prove any of the theorems below, and indeed any of the proofs would be beyond the scope of this course.
Definition: Finite Borel Hierarchy The finite Borel hierarchy consists of two sequences {Σn} and {Πn} of subsets of B defined as follows: • Σ1 is the collection of all open sets in R, and Π1 is the collection of all closed sets in R.
• For each n ≥1, the collection Σn+1 consists of all countable unions of sets from Πn, and the collection Πn+1 consists of all countable intersections of sets from Σn.
For example, Σ2 is the collection of all Fσ sets, and Π2 is the collection of all Gδ sets. Similarly, Σ3 is the collection of all countable unions of Gδ sets, and Π3 is the collection of all countable intersections of Fσ sets. Thus every set in Σ3 can be written Structure of Measurable Sets 14 as [ m∈N \ n∈N Um,n for some open sets Um,n and every set in Π3 can be written as \ m∈N [ n∈N Fm,n for some closed sets Fm,n.
As mentioned in the previous section, every open or closed set is both Fσ and Gδ.
Thus we have Σ1 ⊆Σ2, Σ1 ⊆Π2, Π1 ⊆Σ2, and Π1 ⊆Π2.
Moreover, all four of these inclusions are proper. In particular, Q is in both Σ2 −Σ1 and Σ2 −Π1, and R −Q is in both Π2 −Σ1 and Π2 −Π1. The following theorem generalizes all of this.
Theorem 19 Properties of Σn and Πn For each n ∈N, the following statements hold.
1.
For all S ⊆R, we have S ∈Σn if and only if Sc ∈Πn.
2.
We have Σn ⊆Σn+1, Σn ⊆Πn+1, Πn ⊆Σn+1, and Πn ⊆Πn+1.
Moreover, all four of these inclusions are proper.
If B ⊆R is a Borel set, the Borel rank of B is the minimum n such that B lies in Σn ∪Πn. Thus sets that are open or closed have Borel rank 1, sets that are Fσ or Gδ have Borel rank 2, and so forth.
Amazingly, it is not true that every Borel set has finite rank. For example if {Sn} is a sequence of Borel sets such that each Sn is contained in (n, n+1) and has rank n, then the union S = S1 ∪S2 ∪S3 ∪· · · cannot have any finite rank. Such a set S is said to have rank ω, and the collection of all such sets is known as Σω. The complement of any set in Σω is also said to have rank ω, and the collection of all such sets is known as Πω.
The Borel hierarchy continues even beyond ω. For example, Σω+1 consists of all countable unions of sets from Πω, and Πω+1 consists of all countable intersections of Structure of Measurable Sets 15 sets from Σω. Indeed, we have a sequence of sets Σ1 ⊆Σ2 ⊆Σ3 ⊆· · · ⊆Σω ⊆Σω+1 ⊆Σω2 ⊆· · · ⊆Σ2ω ⊆Σ2ω+1 ⊆· · · and similarly for the Π’s. The result is that the sets Σα and Πα can be defined for each countable ordinal α (i.e. for each element of a minimal uncountable well-ordered set SΩ). The resulting families {Σα}α∈SΩand {Πα}α∈SΩconstitute the full Borel hierarchy, and the Borel algebra B is the union of these: B = [ α∈SΩ Σα = [ α∈SΩ Πα.
Incidentally, it is not too hard to prove that each of the sets Σα and Πα has the same cardinality as R. Since |SΩ| ≤|R|, it follows that the full Borel algebra B has cardinality |R| as well.
Theorem 20 Cardinality of the Borel Algebra Let B be the Borel σ-algebra in R. Then |B| = |R|.
By Corollary 9, the cardinality of the collection of measurable sets is equal to |P(R)|, which is greater than the cardinality of the Borel algebra. This yields the following corollary.
Corollary 21 There exists a Lebesgue measurable set that is not a Borel set.
Since the Borel algebra is a σ-algebra, we could of course restrict Lebesgue measure to the Borel algebra, yielding a measure m|B : B →R. However, this measure is not complete, since there exist Borel sets of measure zero (such as the Cantor set) whose subsets are not all Borel. Indeed, by Proposition 16, Lebesgue measure is precisely the completion of the measure m|B.
Exercises 1. Prove that every nonempty open set has positive measure.
Structure of Measurable Sets 16 2.
a) Let S ⊆R, and let C be a collection of open sets that covers S. Prove that C has a countable subcollection that covers S.
b) A set S ⊆R is locally measurable if for every point x ∈S there exists an open set U containing x so that S ∩U is measurable. Prove that every locally measurable set is measurable.
3. A subset of R is totally disconnected if it does not contain any open intervals (e.g. the Cantor set). Give an example of a closed, totally disconnected subset of [0, 1] that has positive measure.
4.
a) If S ⊆R, prove that m∗(S) = inf{m(E) | E is measurable and S ⊆E}.
b) If S ⊆R, prove that m∗(S) = sup{m(E) | E is measurable and E ⊆S}.
5. Let E ⊆R be a measurable set with m(E) < ∞, and let S ⊆E. Prove that m∗(S) = m(E) −m∗(E −S).
6. If {Sn} is a sequence of pairwise disjoint subsets of R, prove that m∗ ] n∈N Sn ≥ X n∈N m∗(Sn).
7. Prove that a set S ⊆R is Fσ if and only if its complement is Gδ.
8. Prove that every countable subset of R is Fσ.
9. Prove that the intersection of two Fσ sets is Fσ.
10. Prove that every open set is both Fσ and Gδ. Deduce that the same holds true for closed sets.
11. Give an example of a set which is both Fσ and Gδ but is neither open nor closed.
12. Let C be the collection of all uncountable subsets of R. Prove that the σ-algebra generated by C is the power set of R.
13. Prove that the σ-algebra generated by the collection {(a, ∞) | a ∈R} is the Borel sets.
14. Let M be the collection of Lebesgue measurable sets in R. Prove that M is the σ-algebra generated by the open intervals together with all sets of measure zero. |
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Scientific Notation Calculator
The scientific notation calculator will take any decimal value and convert it to scientific notation. Here we will not only tell you what scientific notation is all about but also explain the scientific notation rules and discuss slight variations that might appear in different domains where people use scientific notation.
What is scientific notation?
Scientific notation is generally used with very large or very small numbers in applications such as physics, engineering, and chemistry. It condenses the numbers into a number a between 1 (included) and 10 (excluded) multiplied by 10 raised to an exponent, denoted as a × 10ⁿ.
Scientific notation rules
When converting a number into scientific notation, we must remember a few rules.
First, the decimal point must be between the first two non-zero digits. The number prior to the multiplication symbol is known as the significant or mantissa. The number of digits in the significant depends on the application and are known as significant figures. The significant figures calculator can assist in this situation.
The value of the exponent depends on whether or not the decimal place is moved to the right or left to return to the original number. An example of how to convert a number into scientific notation is done in the next section.
To better understand these rules of scientific notation, let's discuss an example.
How do I convert a number to scientific notation?
Suppose we want to convert 0.00345 to scientific notation:
Place the decimal point between the first two non-zero digits, so we have 3.45.
Count the number of decimal places that were moved, which in this case is 3.
Determine whether the new number (3.45) is larger or smaller than the original (0.00345).
If the new number is larger than the original, then the exponent is negative. If it is smaller, then the exponent is positive.
Write in terms of a × 10ⁿ, in this case, 3.45 × 10-3.
Verify this result with our scientific notation calculator! If you want the answer to have two significant figures, round the significant to 3.5. The rounding calculator is a great tool to accomplish this task. Also helpful in converting numbers to scientific notation is the exponent calculator.
How to use the scientific notation converter
It's very easy to use Omni's scientific notation calculator: just input a number and our converter will do the rest.
Note that this scientific notation converter uses e plus or minus the exponent, instead of 10 raised to the exponent. There are several different notations used, depending on the application. Computer languages, engineering, and mathematical applications use similar but different ways to represent scientific notation.
If you are searching for useful maths calculators do not hesitate to take a look at the cube root calculator which enables you to calculate not only cube root but also roots of any degree.
FAQs
How do I multiply and divide in scientific notation?
Suppose you have two numbers written in scientific notation: a × 10ⁿ and b × 10ᵐ.
To multiply them, multiply the coefficients and add the exponents: (a×b) × 10n+m.
To divide the first one by the second, divide the coefficients and subtract the exponents: (a/b) × 10n-m.
The result need not be in scientific notation! It's recommended you verify if it is and perform the conversion if needed. You may use Omni's scientific notation calculator to do this task quickly and easily.
What is 4,500 in scientific notation?
4.5×10³ or, equivalently, 4.5e3. This is because we want to write 4,500 as a × 10ⁿ with a ∈ [1,10) and n an integer.
What is 0.00057 in scientific notation?
5.7 × 10-4 or, equivalently, 5.7e-4. In this way, we've written our number as a × 10ⁿ with a ∈ [1,10) and n an integer.
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Word of the Day: Intrigue
BySimran Jeet
Apr 12, 2025 02:48 pm
What's the story
The word "intrigue" can be used as both a noun and a verb. As a verb, it means to arouse someone's curiosity or interest. As a noun, it refers to a secret plot or mysterious plan. Whether you're fascinated by a story or caught in a web of mystery, "intrigue" fits both situations perfectly.
Origin
Origin of the word
The word "intrigue" comes from the French word intriguer, which means "to plot or scheme." It was borrowed from the Italian intricare, meaning "to entangle." Over time, English adopted "intrigue" to refer to both mysterious planning and the feeling of being deeply interested or curious about something.
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Synonyms
Synonyms for 'intrigue'
Some common synonyms for "intrigue" include fascinate, captivate, interest, puzzle, bewitch, engage, enthrall, and attract. While many of these words express curiosity or attention, "intrigue" often adds a layer of mystery, making it more suitable for suspenseful or complex situations.
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Usage
Sentence usage
Here are a few examples to show how "intrigue" can be used in everyday language: "The ancient ruins continue to 'intrigue' historians around the world." "There was an air of 'intrigue' around the new neighbor no one had met." "Her unique style and confidence 'intrigued' everyone at the event." "The spy novel was full of 'intrigue' and unexpected twists."
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Writing
Why use the word
Using "intrigue" helps bring depth and curiosity into your speech or writing. It goes beyond simple interest and adds a feeling of mystery or complex attraction. Whether you're writing a story, describing a person, or discussing a mystery, "intrigue" brings richness and suspense to your words.
Done!
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11387 | https://journals.plos.org/ploscompbiol/article?id=10.1371/journal.pcbi.1010998 | Loading metrics
Open Access
Research Article
GenoVi, an open-source automated circular genome visualizer for bacteria and archaea
Andrés Cumsille ,
Contributed equally to this work with: Andrés Cumsille, Roberto E. Durán
Roles Conceptualization, Data curation, Formal analysis, Funding acquisition, Investigation, Methodology, Software, Validation, Visualization, Writing – original draft, Writing – review & editing
Affiliation Laboratorio de Microbiología Molecular y Biotecnología Ambiental, Departamento de Química & Centro de Biotecnología Daniel Alkalay Lowitt, Universidad Técnica Federico Santa María, Valparaíso, Chile
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Roberto E. Durán ,
Contributed equally to this work with: Andrés Cumsille, Roberto E. Durán
Roles Conceptualization, Data curation, Formal analysis, Funding acquisition, Investigation, Methodology, Project administration, Resources, Software, Supervision, Validation, Visualization, Writing – original draft, Writing – review & editing
E-mail: roberto.duranv@usm.cl
Affiliation Laboratorio de Microbiología Molecular y Biotecnología Ambiental, Departamento de Química & Centro de Biotecnología Daniel Alkalay Lowitt, Universidad Técnica Federico Santa María, Valparaíso, Chile
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Andrea Rodríguez-Delherbe,
Roles Data curation, Formal analysis, Investigation, Methodology, Software, Validation, Visualization, Writing – review & editing
Affiliations Radcliffe Department of Medicine, MRC Weatherall Institute of Molecular Medicine, University of Oxford, Oxford, United Kingdom, Departamento de Informática, Universidad Técnica Federico Santa María, Valparaíso, Chile
⨯
Vicente Saona-Urmeneta,
Roles Data curation, Formal analysis, Investigation, Software, Validation, Visualization, Writing – review & editing
Affiliation Departamento de Informática, Universidad Técnica Federico Santa María, Valparaíso, Chile
⨯
Beatriz Cámara,
Roles Resources, Writing – review & editing
Affiliation Laboratorio de Microbiología Molecular y Biotecnología Ambiental, Departamento de Química & Centro de Biotecnología Daniel Alkalay Lowitt, Universidad Técnica Federico Santa María, Valparaíso, Chile
⨯
Michael Seeger,
Roles Funding acquisition, Resources, Writing – review & editing
Affiliation Laboratorio de Microbiología Molecular y Biotecnología Ambiental, Departamento de Química & Centro de Biotecnología Daniel Alkalay Lowitt, Universidad Técnica Federico Santa María, Valparaíso, Chile
⨯
Mauricio Araya,
Roles Conceptualization, Funding acquisition, Writing – review & editing
Affiliation Departamento de Electrónica, Universidad Técnica Federico Santa María, Valparaíso, Chile
⨯
Nicolás Jara,
Roles Conceptualization, Funding acquisition, Writing – review & editing
Affiliation Departamento de Electrónica, Universidad Técnica Federico Santa María, Valparaíso, Chile
⨯
Carlos Buil-Aranda
Roles Conceptualization, Funding acquisition, Project administration, Resources, Supervision, Writing – review & editing
Affiliation Departamento de Informática, Universidad Técnica Federico Santa María, Valparaíso, Chile
⨯
GenoVi, an open-source automated circular genome visualizer for bacteria and archaea
Andrés Cumsille,
Roberto E. Durán,
Andrea Rodríguez-Delherbe,
Vicente Saona-Urmeneta,
Beatriz Cámara,
Michael Seeger,
Mauricio Araya,
Nicolás Jara,
Carlos Buil-Aranda
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Published: April 4, 2023
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Abstract
The increase in microbial sequenced genomes from pure cultures and metagenomic samples reflects the current attainability of whole-genome and shotgun sequencing methods. However, software for genome visualization still lacks automation, integration of different analyses, and customizable options for non-experienced users. In this study, we introduce GenoVi, a Python command-line tool able to create custom circular genome representations for the analysis and visualization of microbial genomes and sequence elements. It is designed to work with complete or draft genomes, featuring customizable options including 25 different built-in color palettes (including 5 color-blind safe palettes), text formatting options, and automatic scaling for complete genomes or sequence elements with more than one replicon/sequence. Using a Genbank format file as the input file or multiple files within a directory, GenoVi (i) visualizes genomic features from the GenBank annotation file, (ii) integrates a Cluster of Orthologs Group (COG) categories analysis using DeepNOG, (iii) automatically scales the visualization of each replicon of complete genomes or multiple sequence elements, (iv) and generates COG histograms, COG frequency heatmaps and output tables including general stats of each replicon or contig processed. GenoVi’s potential was assessed by analyzing single and multiple genomes of Bacteria and Archaea. Paraburkholderia genomes were analyzed to obtain a fast classification of replicons in large multipartite genomes. GenoVi works as an easy-to-use command-line tool and provides customizable options to automatically generate genomic maps for scientific publications, educational resources, and outreach activities. GenoVi is freely available and can be downloaded from
Author summary
Genome visualization tools can inspect genomic features in a DNA sequence, delivering a visual aid to quickly understand genome architecture and function. Circular representations frequently display the GC content, useful to identify genomic islands and horizontal gene transfer events; GC skew, the over or under abundance of G or C between the leading and lagging DNA strands frequently used to identify the origin and terminus of replication; coding DNA sequences (CDS), and Clusters of Orthologous Groups (COGs) to classify predicted CDS for functional studies. However, genome visualization tools frequently require these features in specific formatting as input, hampering their usage, and lacking versatility for comparative genomics purposes. GenoVi uses an annotated genome file as input, automatically calculates each of the aforementioned genomic features, and generates a ready-to-use figure in minutes. Additionally, GenoVi has many customizable format options and works with complete, draft, and multiple genomes useful for comparative genomics applications.
Citation: Cumsille A, Durán RE, Rodríguez-Delherbe A, Saona-Urmeneta V, Cámara B, Seeger M, et al. (2023) GenoVi, an open-source automated circular genome visualizer for bacteria and archaea. PLoS Comput Biol 19(4): e1010998.
Editor: Ilya Ioshikhes, CANADA
Received: August 29, 2022; Accepted: March 5, 2023; Published: April 4, 2023
Copyright: © 2023 Cumsille et al. This is an open access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
Data Availability: GenoVi is freely available under a BY-NC-SA Creative Commons License and can be downloaded from GenoVi can be obtained in two steps: Creating a Conda environment with Circos, followed by installation using the package-management system pip with pip install genovi. Also, a Docker container of GenoVi is available. Genomes used in this study are available at
Funding: This work was supported by USM_PI_M_43 Proyecto USM Multidisciplinarios 2020, - Universidad Técnica Federico Santa María (UTFSM; A.C., R.E.D., V.S.-U., M.A., N.J., C.B.-A.), Fondecyt 1200756 - Agencia Nacional de Investigación y Desarrollo (ANID; M.S., R.E.D.), and ANID -- Millennium Science Initiative Program -- Code ICN17_002 (C.B.-A.) grants. A.C. was supported by ANID 21191625 PhD fellowship and Programa de Incentivos a la Iniciación Científica, UTFSM. The funders had no role in software design, data collection or analysis, decision to publish or the preparation of the manuscript.
Competing interests: The authors have declared that no competing interests exist.
This is a PLOS Computational Biology Software paper.
Introduction
The growth of genomic data has resulted in more than 250,000 unique bacterial and archaeal genomes available in public databases since the first genome was sequenced [1,2]. Large-scale projects, international research collaborations, and smaller groups employ genomics and environmental genomics to pursue new knowledge and understand complex questions in evolution, ecology, systematics, biomedical sciences, and other areas, generating extensive amounts of data while discovering new patterns and mechanisms within life sciences . Metagenome-assembled genomes (MAGs), which are increasing day-by-day due to metagenomic studies , as well as the current genome sequencing accessibility for most research groups, build up the need to create automated and easy-to-use tools to analyze and interpret its information.
Circular genome visualization is a widely used method for data analysis and representation of genomic elements. General features usually displayed in a circular representation includes the GC content, the guanine and cytosine uneven proportion in the two DNA strands, phenomenon called GC skew , classification of proteins into Clusters of Orthologous Groups of proteins (COGs) [5,6], and the location of tRNAs and rRNAs in the genome. Different tools are available for circular genome visualization, such as CGView , CiVi , DNAPlotter , Circleator , and Circos . However, their usage often accepts only complete chromosomes or plasmids for circular representation (Table 1). Others require programming skills for the creation of complex intermediate and configuration files increasing the gap between users and graphical visualization. Complementary analyses for genome visualization, such as COGs classification and configuration files, as well as custom colors, are not easy to achieve, hampering their implementation in visualization tools (Table 1) .
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Table 1. Comparison of circular genome visualization software.
This work presents GenoVi, a Python-based tool that automatically formats each file to create a circular representation of bacterial or archaeal genomes integrating multiple tools. GenoVi displays COGs annotation, coding DNA sequences (CDS), GC content, GC skew, tRNA, and rRNA localization using a GenBank format file (gbff, gbk, gb) as an input file. This tool bypasses the difficulties associated with data processing, specific formatting such as the configuration files required by Circos and several customization options, delivering a high-quality figure using complete or draft genomes. Additionally, GenoVi creates output files with COGs classification information in minutes, as well as general features tables, making it useful for single genome representation, and comparative genomic studies.
Design and implementation
GenoVi is a command-line tool that compiles different software to create a ready-to-publish circular genome representation. GenoVi automatically calculates the GC content and GC skew from a genome, and unless specified, assigns CDS to COG categories. As additional resources, GenoVi produces histograms, heatmaps and tables of COG categories and frequency, and a table with general information about each contig/replicon, including size, GC content, number of CDS, tRNAs, and rRNAs. The originality of GenoVi resides in being a one-step, and easy-to-use tool that computes all the information needed to create a customizable genome representation in a matter of minutes, using as input an annotated genome. GenoVi can be used for single genome visualization or for comparative genomic studies.
GenoVi workflow
As input, GenoVi uses a Genbank format file (gbff), which is converted into a nucleotide fasta (.fna) using a modified version of genbank2fasta tool. Then, the fasta file is used to calculate the GC content using a script based on GC-analysis.py , and the GC skew using SkewIT for any sequence element identified in the input file . In both cases, GenoVi uses a user-specified window size for calculation (default = 1,000 bp). Concurrently, from the original gbff file, GenoVi obtains the position of CDS, tRNA, and rRNA associated with each sequence element.
As a default feature, GenoVi parses the gbff file into a protein fasta (.faa) to predict and classify each CDS into COG categories using the COG 2020 database. This feature is accomplished using DeepNOG, a fast alignment-free method based on convolutional network architecture achieved within a few minutes. . After calculating each genomic feature, GenoVi creates configuration files needed to display a circular representation using Circos. In addition, GenoVi delivers as output a histogram of COG categories abundance, a heatmap of COG frequency per contig/replicon, and three output tables: COG classification raw data, COG percentage distribution per genome/replicon, and general features which could be used for further analyses.
Usage
GenoVi is a Python-based command-line software installed by creating a Circos containing Conda environment . GenoVi can then be installed through pip, which also incorporates DeepNOG , and Python libraries (NumPy, Pandas, Biopython, Matlibplot, and CairoSVG). GenoVi can also be installed from our git repository, previously installing each dependency.
GenoVi relies upon user indication of the input file and the genome status (“draft” or “complete”; Fig 1A). For our purposes, draft genomes are DNA assemblies fragmented in contigs or scaffolds interspersed with gaps of unknown length, whereas complete genomes have defined length gaps filled with “N” (any nucleotide) or no gaps, in which each scaffold represents an independent replicon (e.g. chromosome, chromid, megaplasmid or plasmid). We encourage to use complete genomes with N-filled gaps assemblies only when necessary, due to the inability to obtain genomic features from that data. The genome status argument defines two main methods for visualization: -draft, incorporating each scaffold as bands in the same unique circular representation; and -complete where each scaffold is treated separately to generate a circular representation. Genovi can also use directories containing several genomes as an input, treating each genome individually as draft or complete depending on the user selection, useful for comparative genomic analysis.
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Fig 1. Overview of GenoVi workflow.
(A) GenoVi incorporates several customizable options for visualization, such as an option for complete or draft genomes, twenty-five prebuilt color palettes, title, scale-up options, and COG categories selection. (B) GenoVi uses Genbank format files (gbff) as input. From each file GenoVi extracts CDS and RNAs position. Additionally, GenoVi converts this file into a nucleotide FASTA to calculate GC content, GC skew, and, if user-specified, into a protein FASTA to classify into COGs categories. (C) After calculating and formatting each genomic feature, GenoVi uses Circos to build a genome representation in svg and png format. COG abundance histogram, COG frequency heatmaps and summarizing tables of overall genomic features are also created in this step.
GenoVi can be used with genbank format files from official annotators of the International Nucleotide Sequence Database Collaboration (Fig 1B), including the NCBI Prokaryotic Genome Annotation Pipeline from GenBank and the DDBJ Fast Annotation and Submission Tool (DFAST) from the DNA Database of Japan (DDBJ; ), as well as annotation files from Prokka .
GenoVi has several user-customizable options. Color selection for CDS, GC content, GC skew, tRNA, rRNA, font, and background. Additionally, GenoVi includes twenty-five pre-built color palettes suitable for visual representation of microbial genomes from different environments or contexts, including five color-blind friendly palettes. A figure title and replicon size display option are available. Additionally, italicized words in the title can be added for precise taxonomic nomenclature. For complete genomes with more than one replicon, e.g., one chromosome and plasmids, three scaling options (viz. variable, linear, sqrt) are offered. This option is especially useful for genome containing broad differences in replicon size which could affect the illustration of small sequence elements (Fig 1A).
To enhance and customize the genomic feature estimations, the user can specify the window size in bp for GC content and GC skew calculations, and the confidence threshold for DeepNOG COGs classification. To avoid re-processing when deciding image preferences, two options are available: keep temporary files (-k), and reuse COG annotation performed by DeepNOG (-r). COGs categories can be selectively displayed using the—cogs argument, choosing specific categories (—cogs EMX), a group of COG categories (—cogs inf-, for Information Storage and Processing: ABJKLX) or the N-most abundant COGs identified (—cogs #, representing a numerical value of top categories to be displayed). Genomic maps created by GenoVi are obtained as PNG and SVG files (Fig 1C), which could be further edited in vector files editing programs such as Adobe Illustrator, Inkscape, Vector, or Microsoft PowerPoint.
GenoVi outputs tables and visualizations are suitable to be used as single genome representation figures, as well as for comparative genomic studies.
Results and discussion
GenoVi can be used to visualize and analyze data obtained from (i) draft genomes, (ii) complete genomes, (iii) and multiple genomes, converting it into a suitable tool for single and comparative genomics.
To perform genome visualization and analysis of a genomic sequence, a keyword feature is available to indicate whether the DNA is completely sequenced or in draft status. For draft genomes (Fig 2A), GenoVi creates one map that includes each scaffold or contig in the same circular plot. The genome of the type strain of Corynebacterium alimapuense VA37-3T [Accession Number: GCF_003716585.1; 18] was used as an example. Genome assembly yielded 12 contigs, where five hold most of the genomic information (Fig 2A). The total assembly length is 2.3 Mb, and has a GC content of 57%, standing slightly above the average of the genus (~55%) . The most representative COG categories in strain VA37-3T are J (translation, ribosomal structure, and biogenesis), E (amino acid transport and metabolism), and R (general function prediction only). Similar results were obtained in Corynebacterium diphtheriae strains, where E and J COG categories were the most abundant .
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Fig 2. Application of GenoVi using a draft or complete bacterial genome.
(A) GenoVi circular map of the draft genome of Corynebacterium alimapuense VA37-3T (-s draft -cs paradise). Each contig is represented as separated bands of one circular representation. (B) GenoVi circular representation of the complete genome of Acinetobacter radioresistens DD78 (-s complete, -cs autumn). Each circular map represents a replicon from the complete genome. A. radioresistens DD78 genome consists of a circular chromosome and three circular plasmids displayed next to the chromosome (—scale variable). Labeling from outside to the inside: Contigs; COGs on the forward strand; CDS, tRNAs, and rRNAs on the forward strand; CDS, tRNAs, and rRNAs on the reverse strand; COGs on the reverse strand; GC content; GC skew.
GC skew is the guanine-cytosine asymmetry observed when comparing the leading and lagging DNA strands in a continuous sequence. Graphical representation or cumulative GC skew plots shows an inflection point used to identify the origin and terminus (ori/ter) of replication in bacteria. Also, mean GC skew values tend to be rather similar across bacterial genera, being a good method to identify misassemblies [4,20]. Due to the draft nature of strain VA37-3T assembly, GC skew only reveals which contigs harbor a possible ori/ter (Fig 2A).
For complete genome visualization, GenoVi creates a circular map for each replicon in the input file, assuming that each continuous sequence is independent. GenoVi scales each representation according to its length, providing the option to choose different scaling algorithms. Acinetobacter radioresistens DD78 [Accession Number: GCF_005519305.1; 21] (Fig 2B) was used as a complete genome example with multiple replicons. The chromosome is 3.0 Mb and has a GC content of 41.8%. In contrast, the three plasmid sizes are 88.5 kb, 80.1 kb, and 69.2 kb with a GC content of 38.9%, 40.7%, and 37.1%, respectively. The overall GC content is 41.6% which is above the average of the genus of 39.4%. The GC skew of strain DD78 shows two inflection points where possibly the origin and the terminus are located (Fig 2B) . The most abundant COG categories were R, J, and M (cell wall/membrane/envelope biogenesis). These results are distant from those reported for Acinetobacter venetianus VE-C3, which reports a majority in the L (replication, recombination, and repair) COG category . Strain DD78 possesses 77 tRNAs and 21 rRNAs, all located at the chromosome (Fig 2B).
For a comprehensive display of COG categories, GenoVi holds several options for COG representation. Otherwise stated using the—cogs argument, every COG category will be illustrated (Figs 2 and 3A). The complete genome of the Crenarchaeota, Sulfolobus acidocaldarius DG1 (GCA_002215565.1, -s complete -cs paradise) is illustrated (Fig 3A). Selecting only the most abundant 5 COGs within the DG1 genome, we can observe a high density of J and K (Replication) orthologs in the region between 400 and 550 kb (—cogs 5; Fig 3B). When only displaying CDS classified as J orthologs, we can observe that most genes within that range encode for proteins related to translation, ribosomal structure, and biogenesis processes (—cogs J; Fig 3C). Selective COG display as seen in the genome of strain DG1, allows the analysis and location of specific functional categories within each genome depicted.
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Fig 3. High density of Translation, ribosomal structure and biogenesis (J) orthologs is located in the region 400–500 kb of Sulfolobus acidocaldarius DG1 genome.
(A) Genovi representation of the complete genome of S. acidocaldarius DG1 is depicted using default parameters (-s complete -cs paradise). (B) Most abundant five COG categories within the 400–550 kb range of DG1 genome are represented (—cogs 5), which included C (Energy production and conversion), E (Amino acid transport and metabolism), J (Translation, ribosomal structure, and biogenesis), K (Transcription) and R (General function prediction only). (C) Genovi representation of J category orthologs within the 400–550 kb genome of S. acidocaldarius DG1 (—cogs J).
The display of specific COG categories can facilitate genome mining of biosynthetic gene clusters (BGCs) containing large CDS. The genome of strain Rhodococcus sp. H-CA8f (GCF_002501585.1) comprises two replicons, a chromosome of 6.19 Mb and a plasmid of 301 Kb (Fig 4. ). Genome mining analysis of this strain rendered the presence of 17 BCGs, six of which are non-ribosomal peptide synthetases (NRPSs), highly relevant for the production of specialized metabolites, such as antimicrobials . NRPSs are modular multidomain enzymes which have been reported to be the most prevalent classes of BGCs in Nocardia , as well as in Rhodococcus [24,26]. NRPS BGCs in strain H-CA8f range from 55.5 Kbp to 98.4 Kbp , where the core biosynthetic genes range from 12.4 Kbp to 26.9 Kbp. The genome of strain H-CA8f was represented displaying only the COG category Q (secondary metabolites biosynthesis;—cogs Q; Fig 4). The presence of the six NRPS BGCs from this strain are highlighted and are easily observable, demonstrating that GenoVi could be a useful tool to quickly display the presence of genes that encode for megaenzymes.
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Fig 4. Visualization of NRPS biosynthetic gene clusters within the genome of Rhodococcus sp. H-CA8f.
Genovi representation of Rhodococcus sp. H-CA8f complete genome is depicted with an interior break in the ideogram to easily identify each track (-s complete, -cs dawn,—cogs Q, -te). Selection of Q orthologs (Secondary metabolites biosynthesis, transport, and metabolism) within the H-CA8f genome includes NPRS CDSs and can be easily seen by the whole genome representation.
Visualization and analysis of multiple genomes: Paraburkholderia
To address the potential of GenoVi for comparative genomics, a directory containing multiple genomes can be given as input. Each file will be analyzed independently, following the normal workflow of the tool. Output tables describing the genomic features and COG information of each genome analyzed can be of great support for comparative genomics studies. When multiple genomes are given as an input, GenoVi processes each file independently and creates tables summarizing the general statistics, COG identification and COG frequency of every genome analyzed into one file.
To better illustrate the usage of the output tables rendered by GenoVi, a genomic analysis was performed on 36 complete genomes of Paraburkholderia to identify genomic traits for its replicon classification (S1 Text and S1 Table). Paraburkholderia is a bacterial genus encompassing strains often isolated from plant, insect, soil, and anthropogenic-impacted sites [27–29]. Diverse pollutant-degraders and plant-growth-promoting bacteria (PGPB) are part of this taxon, including the degrader of polychlorobiphenyls and aromatic compounds Paraburkholderia xenovorans LB400T , BTEX and hydrocarbon degrader Paraburkholderia aromaticivorans BN5T , and the PGPB model bacteria Paraburkholderia phytofirmans PsJnT .
Paraburkholderia is characterized by multipartite genomes comprised of at least two large replicons, a larger element referred to as chromosome or first chromosome in some studies (C1), and a chromid generally designated as the second chromosome (C2). Other genetic elements are usually detected in the genus, including other possible chromids or megaplasmids, classified into each type depending on the presence of indispensable genes for cellular viability. Plasmids are also generally encountered in Paraburkholderia genomes [31,33]. Chromosome identification is an easy task, as the genetically stable largest replicon, while chromid—megaplasmid—plasmid categories are not as easily distinguished. Corroboration of core genes, plasmid-type maintenance and replication proteins, codon usage, size, GC-content, and dinucleotide relative abundance distance have been used as markers to classify replicons into chromids, megaplasmids, or plasmids in multipartite genomes [34–36]. Intricate classification boundaries, more than three replicons in most of Paraburkholderia, and a wide size range translate into a non-trivial replicon classification in Paraburkholderia, leading to misclassifications. While the misidentification of a replicon type does not imply an error for general genomic studies, an easier approach could facilitate the study of the evolutionary relatedness across replicons from the same taxa, the relevance of inter-replicon transcriptional regulation, and the essential nature of any of the replicons within an organism [34,35].
Previous studies have reported differential COG distribution across replicons of P. xenovorans LB400T and other bacteria, describing functional patterns per replicon [30,33,37,38]. diCenzo et al, corroborated a functional bias between each replicon class regardless of their phylogeny, highlighting the presence of transposable elements in plasmids . These data suggest that COG distribution patterns across replicons could be used as an effective tool to quickly identify overall genetic functions, facilitating replicon classification into chromosomes, chromids, megaplasmids, or even plasmids.
COG percentage distribution differentiates three major groups within Paraburkholderia multipartite genomes
A total of 146 replicons ranging from 22 kb to 4.94 Mb, from 36 complete genomes were analyzed by GenoVi (S1 Table) [30–32,39–53]. Hierarchical clustering analysis of COG percentage distribution was evaluated to assess functional bias relevance to replicon classification in Paraburkholderia (Fig 5A). COG patterns showed three major groups, where the group designated as “Chromosomes” (n = 36) and “Chromids and megaplasmids” (n = 75) displayed a more conserved functional pattern, while the class designated as “plasmids” (n = 35) did not possess a clear functional organization besides a general enrichment in the COG class X (Mobilome: prophages, transposons) (Fig 5A and S1 Fig). As expected, only the largest replicon from each genome analyzed is encountered in chromosomes (Fig 5A and S1 Fig). The second larger replicon was always allocated in the chromids and megaplasmid group, alongside other large secondary replicons and megaplasmids (e.g., strain LB400 megaplasmid) confirming the functional bias in Paraburkholderia secondary large replicons already observed in other multipartite genomes .
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Fig 5. COG percentage distribution of Paraburkholderia replicons elucidates general functional patterns useful for its classification.
(A) COG percentage distribution of the 146 replicons from the Paraburkholderia genus. Hierarchical clustering revealed three distinct groups: Major chromosomes C1 (red); Minor chromosomes C2-C3-C4-C5-p1 (green); Plasmids (blue). CP&S: Cellular Processes and Signaling; IS&P: Information Storage and Processing; PC: Poorly Characterized. (B). Genomic features (size, GC-content, tRNA, and rRNA) from each replicon type were identified by COG percentage distribution. tRNA is the best feature to identify chromosomes (C1).
Overall genomic features from each replicon type emphasize the segregation of the three groups, observing statistical differences (p<0.001) in size, GC-content, tRNAs, and rRNAs among every group (Fig 5B). However, only the presence of a complete tRNAs repertoire (>50) can be used as a specific marker for identification of chromosomes. Other general features, such as size or GC-content can be helpful to guide the identification of chromosomes or plasmids, but some outliers in each group hamper their usage as specific markers.
In general, Paraburkholderia chromosomes possess a similar pattern in comparison to chromids and megaplasmids, with only a few COG categories showing significant differences between both groups (Fig 5 and S2 Fig). Regardless, the COG category J has an average representation of 6.08 ± 0.59% in chromosomes, while in chromids-megaplasmids is about 1.92 ± 0.93%, adding another signature feature to distinguish between chromosomes and other secondary large replicons (Fig 5). Chromids and megaplasmids of Paraburkholderia have a higher COG category K, associated with additional transcriptional regulation mechanisms part of larger secondary replicons (S2 Fig).
Discrimination between plasmids and megaplasmids has been delimited by setting an arbitrary boundary size (~350 kb) which may consider megaplasmids as large plasmids that do not follow some other features of this replicon type . While functional distribution cannot identify a similar copy number than chromosomes or an independent partitioning system, it can discern which replicons are distantly related and functionally unstable in relation to the chromosomes and chromids from Paraburkholderia, indicating at least remote large and small plasmids in the taxa. For the extent of our analysis, plasmids were defined as replicons distantly related to chromosomes, chromids, and megaplasmids in terms of functional organization independently of their size. The group is composed of sequence elements ranging from 22 kb to 971 kb (Fig 5B), mainly enriched in the new COG category X, including transposases, integrases, and other mobile elements incorporated in the last update of the COG database 2020 . Categories D (Cell cycle control, cell division, chromosome partitioning) and L are also higher in this group than other replicon types, while categories associated with amino acid and coenzyme transport/metabolism (E and H) are less represented in comparison to chromosomes, chromids or megaplasmids (Fig 5A and S2 Fig).
Paraburkholderia terrae KU-15 complete genome is displayed as an example to quickly identify and classify each replicon type using general features and functional profiling delivered by GenoVi (Fig 6; ). The genome architecture of strain KU-15 is comprised by six replicons, the chromosome (3.74 Mb) and five other replicons of 2.88 Mb, 2.29 Mb, 754.53 kb, 692.03 kb and 64.71 kb (Fig 6A). COG categories are differentially enriched in each replicon displayed by the heatmap obtained by GenoVi. The first replicon (chr1) is the largest, enriched in J orthologs, as commonly seen for other chromosomes (Fig 6B). Replicons chr2 and chr3 possess a higher proportion of K and R categories, a characteristic of chromids and megaplasmids. Chr6 is the smallest replicon, possessing a much higher L and X categories. Interestingly, chr4 and chr5 also exhibited functional patterns usually found on plasmids (Fig 6B).
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Fig 6. Paraburkholderia terrae KU-15 visualization and analysis by GenoVi allows its replicon classification.
(A) Complete genome representation of P. terrae KU-15 using the blossom palette (-cs blossom). (B) Heatmap generated by GenoVi representing COG percentage frequency of each replicon of P. terrae KU-15 genome. Red boxes highlight key COG categories to differentiate each replicon type.
General features and functional profiling of Paraburkholderia replicons can help to quickly guide the identification of chromosomes, chromids, and megaplasmids within this taxon, although thresholds based on experimental validation are needed to set up accurate boundaries for their classification. Nevertheless, the development of bioinformatic tools that help researchers to easily obtain genome profiling data allows us to identify patterns shedding novel evidence about genome evolution, organization, and architecture within bacterial and archaeal genomes.
GenoVi uses a single input file and creates a customizable circular genomic map in one step, including a built-in COG categories analysis by alignment free-methods, generating a scaled circular representation for complete genomes or multiple replicons, and, therefore, delivering genomic data for comparative genomics analyses, and ready-to-publish circular representations.
Conclusion
GenoVi is an open-source and easy-to-use Python command-line application for the creation of custom circular genome representations of complete and draft genomes, and multiple replicons of bacteria and archaea. It allows COG categories analysis via alignment-free methods, and automatic scaling for complete genomes, which provide the easy visualization of genomic features. Genomic features and COG distribution patterns obtained by GenoVi, are a useful method to quickly discriminate between replicon types in multipartite genomes, as corroborated in the complete genomes from Paraburkholderia.
Availability and Future Directions
GenoVi is freely available under a BY-NC-SA Creative Commons License and can be downloaded from GenoVi can be obtained in two steps: Creating a Conda environment with Circos, followed by installation using the package-management system pip with pip install genovi. Also, a Docker container of GenoVi is available. Genomes used in this study are available at The software is open and we expect researchers to implement it in their routine genomic analyses, being able to request new features that could be implemented. Nevertheless, our team is invested in delivering an interactive web-platform to improve usability for users in biological sciences, which can easily analyze and visualize MAGs or genomic data of single microorganisms, including new modules to highlight a specific loci or locus in the sequence, or adding extra annotation tools that could be useful for environmental or clinical fields.
Supporting information
S1 Fig. Functional distribution patterns show three major groups of the 147 replicons from the Paraburkholderia genus.
Hierarchical clustering of COG percentage shows three major groups in Paraburkholderia replicons.
(TIF)
S2 Fig. Functional distribution per replicon type represented by COG percentage.
(TIF)
S1 Table. General features of Paraburkholderia genomes used in this study.
(PDF)
S1 Text. Supplementary methods.
(DOCX)
Acknowledgments
We kindly thank Leonardo Zamora for his contribution to software validation.
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11388 | https://www.onelook.com/?loc=dmapirel&w=shed | Usually means: A small simple storage building
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We found 45 dictionaries that define the word shed:
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shed: Cambridge Essential American English Dictionary
she'd, shed, shed: Oxford Learner's Dictionaries
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shed, shed, shed: Green’s Dictionary of Slang
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SHED: Power Engineering
(Note: See shedded as well.)
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| Definitions from Wiktionary (shed) ▸ verb: (transitive, obsolete, UK, dialectal) To part, separate or divide. ▸ verb: (ambitransitive) To part with, separate from, leave off; cast off, cast, let fall, be divested of. ▸ verb: (transitive, archaic) To pour; to make flow. ▸ verb: (transitive) To allow to flow or fall. ▸ verb: (transitive) To radiate, cast, give off (light). ▸ verb: (obsolete, transitive) To pour forth, give off, impart. ▸ verb: (obsolete, intransitive) To fall in drops; to pour. ▸ verb: To sprinkle; to intersperse; to cover. ▸ verb: (weaving) To divide, as the warp threads, so as to form a shed, or passageway, for the shuttle. ▸ noun: (weaving) An area between upper and lower warp yarns through which the weft is woven. ▸ noun: (obsolete) A distinction or dividing-line. ▸ noun: (obsolete) A parting in the hair. ▸ noun: (obsolete) The top of the head. ▸ noun: (obsolete outside of compounds) An area of land as distinguished from those around it. ▸ noun: A slight or temporary structure built to shade or shelter something; a structure usually open in front; an outbuilding, especially a smallish one; a hut. ▸ noun: A large temporary open structure for reception of goods. ▸ noun: (British, derogatory, informal) An automobile which is old, worn-out, slow, or otherwise of poor quality. ▸ noun: (British, rail transport, informal) A British Rail Class 66 locomotive. ▸ noun: (nuclear physics) A unit of area equivalent to 10⁻⁵² square meters. ▸ verb: (transitive) To place or allocate a vehicle, such as a locomotive, in or to a depot or shed. ▸ verb: (transitive, music) To woodshed. ▸ noun: A surname. ▸ noun: (music, slang) Alternative form of woodshed. [An enclosed, roofed structure, often an outbuilding, used primarily to store firewood.] Similar: spill, cast, drop, moult, pour forth, exuviate, throw, cast off, shake off, throw away, more... Opposite: accumulate, collect, gather, hoard, retain Types: barn, garage, outhouse, greenhouse, barnacle, cocoon, chrysalis, nest, more... Phrases: shed tears, shed blood, blood shed, tool shed, garden shed, more... Adjectives: old, new, tear, great, large, little, rustic, pull, young, oily, cow Colors: rust, brown, green, gray, red, more... Found in concept groups: --- | | | | | | --- --- | | | | | | --- --- | | | | | --- | | ↻ | From Jenny Wren (Mother Goose rhyme): | | | | As little Jenny Wren Was sitting by her shed. She waggled with her tail, And nodded with her head. | --- 1 of 100+ verses | | | | | ▸ Word origin ▸ Words similar to shed ▸ Usage examples for shed ▸ Idioms related to shed ▸ Wikipedia articles (New!) ▸ Popular adjectives describing shed ▸ Words that often appear near shed ▸ Rhymes of shed ▸ Invented words related to shed |
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| Similar: spill, cast, drop, moult, pour forth, exuviate, throw, cast off, shake off, throw away, more... Opposite: accumulate, collect, gather, hoard, retain Types: barn, garage, outhouse, greenhouse, barnacle, cocoon, chrysalis, nest, more... Phrases: shed tears, shed blood, blood shed, tool shed, garden shed, potting shed, shed roof, cattle shed, train shed, cow shed, shearing shed, transit shed, engine shed, goods shed, boat shed, milking shed, shed roofs, more... Adjectives: old, new, tear, great, large, little, rustic, pull, young, oily, cow Colors: rust, brown, green, gray, red, more... |
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11389 | https://pmc.ncbi.nlm.nih.gov/articles/PMC6570638/ | A retrospective review of 14 cases of malignant otitis externa - PMC
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J Otol
. 2019 Jan 8;14(2):63–66. doi: 10.1016/j.joto.2019.01.003
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A retrospective review of 14 cases of malignant otitis externa
Saldanha Marina
Saldanha Marina
1 Department of Otorhinolaryngology, K.S.Hegde Medical Academy, Nitte(deemed to be University), Mangalore, Karnataka, India
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1,∗, MK Goutham
MK Goutham
1 Department of Otorhinolaryngology, K.S.Hegde Medical Academy, Nitte(deemed to be University), Mangalore, Karnataka, India
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1, A Rajeshwary
A Rajeshwary
1 Department of Otorhinolaryngology, K.S.Hegde Medical Academy, Nitte(deemed to be University), Mangalore, Karnataka, India
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1, Bhat Vadisha
Bhat Vadisha
1 Department of Otorhinolaryngology, K.S.Hegde Medical Academy, Nitte(deemed to be University), Mangalore, Karnataka, India
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1, T Devika
T Devika
1 Department of Otorhinolaryngology, K.S.Hegde Medical Academy, Nitte(deemed to be University), Mangalore, Karnataka, India
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1
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1 Department of Otorhinolaryngology, K.S.Hegde Medical Academy, Nitte(deemed to be University), Mangalore, Karnataka, India
∗
Corresponding author. saldanhamarina@gmail.com
Received 2018 Sep 21; Revised 2018 Dec 28; Accepted 2019 Jan 8; Issue date 2019 Jun.
© 2019 PLA General Hospital Department of Otolaryngology Head and Neck Surgery. Production and hosting by Elsevier (Singapore) Pte Ltd.
This is an open access article under the CC BY-NC-ND license (
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PMCID: PMC6570638 PMID: 31223303
Abstract
Background
Malignant otitis externa is an inflammatory condition of the external ear which has the propensity to spread to the skull base. It can be a difficult entity to treat as clinical presentation varies and response to treatment differs between patients. We reviewed cases of malignant otitis externa in our setup to document the epidemiology and outcome of management.
Methods
This is a retrospective case review observational study from January 2013–December 2017. Fourteen patients diagnosed with malignant otitis externa in our tertiary referral centre were included in the study. Based on hospital protocol, empiric treatment was started. After discharge, the patients follow up visits to the hospital were also documented.
Results
Otalgia was the most common symptom. Edema and congestion of the external auditory canal were observed in most cases. Diabetes was present in all patients. Three cases had associated facial palsy, and one patient had involvement of 7th, 9th, 10th, 11th and 12 th cranial nerve. Two patients with facial palsy recovered. Pseudomonas aeuroginosa was the most common organism isolated (50%).
Conclusions
In our series, malignant otitis externa invariably presented with severe otalgia. Lower cranial palsies were also seen. Methods to evaluate complete eradication of disease should be centered on clinical symptoms and signs, but the measurement of erythrocyte sedimentation rate or radiological imaging may be used as a useful adjunct when there is uncertainty.
Keywords: Malignant otitis media, Granulation tissue, Pseudomonas aeuroginosa, Diabetes
1. Introduction
Malignant otitis externa (MOE) is an infection of the external auditory canal which can spread to the mastoid process and skull base (Singh et al., 2005). Severe otalgia, purulent ear discharge are the common symptoms at presentation. On otoscopic examination, this condition has clinical signs similar to otitis externa; however, the presence of edema and granulations at the osseo-cartilaginous junction in the external auditory canal are more in favor of MOE (Ali et al., 2010). The ability of this disease to spread through the skull base increases its propensity to present with nerve palsies, the facial nerve being the most common nerve involved, followed by other cranial nerve palsies (IX, X, XII). This disease is mostly seen in patients with diabetes and immunocompromised status. The most common organism isolated is Pseudomonas aeruginosa and the widely accepted empiric treatment based on studies is third-generation cephalosporins and fluoroquinolones (Singh et al., 2005; Franco-Vidal et al., 2007; Vadish et al., 2015). It has been noted that some patients do not respond to this treatment and in those cases, fungal MOE due to Aspergillus should be kept in mind and biopsy should be sent to rule out the same (Hasibi et al., 2017). Once the patient is symptomatically better, the otolaryngologist faces the dilemma as to when to stop the medications and prevent the chances of recurrence. In this aspect radionuclide scans, i.e., Gallium- 67- citrate (67 Ga) or 111Indium (111 In) play a significant role as they identify areas of residual infection and these scan return to normal when the infection subsides (Courson et al., 2014).
We aimed to evaluate the clinical presentation and response to treatment in patients who presented to our tertiary referral hospital with malignant otitis externa.
2. Materials and methods
A retrospective observational study from 2013 to 2017 conducted in a tertiary referral hospital. Ethical clearance was obtained from the K.S.Hegde Institutional Ethics committee, Mangalore, India. Identifying information was not documented, and all the data recorded was kept confidential. The case records were reviewed, and 14 patients with malignant otitis externa were identified.
Data recorded was.
1.
Time of presentation after the onset of symptoms
2.
Presenting symptoms
3.
Presenting signs
a.External auditory canal edema and congestion
b.Granulations
c.Tympanic membrane
4.
Organism isolated
5.
Treatment started according to the protocol
6.
Imaging studies- High resolution Computed Tomography (HRCT)Temporal Bone
7.
Erythrocyte sedimentation rate (ESR), Haemoglobin and HbA1c pre-treatment and ESR post-treatment.
8.
Response to treatment was based on the reduction of pain and otoscopy/examination under microscope to examine for a decrease in canal wall edema, congestion, and granulations.
The treatment protocol in our hospital is to start with Injection Ceftazidime 1 gm thrice a day as the monotherapy and then depending on the culture sensitivity report we continue or add other antibiotics. After commencement of treatment, patients who showed improvement regarding the reduction of pain and decrease in ear discharge within two weeks were discharged. These patients were advised acetic acid ear drops and oral/intravenous antibiotics depending on the sensitivity report. They were called for follow up one week after discharge. Patients whose symptoms persisted, and depending on the extent of involvement, local debridement was done.
2.1. Statistical analysis
The data collected was entered into Microsoft Excel spreadsheet and analyzed using IBM SPSS Statistics Version 22 (Armonk, NY: IBM Corp). Frequency and percentage were calculated for the demographic profile, clinical and laboratory characteristics of the patients.
3. Results
Fourteen patients, thirteen males and one female with malignant otitis externa were included in the study. The ages ranged from 43 to 81years (mean, 60 years).
3.1. Clinical presentation
Otalgia was the most common symptom at presentation. Patients presented within 20 days to 4 months after the onset of otalgia. Further details of the clinical symptoms and signs are shown in Table 1. Facial palsy was observed in three patients and one patient who was 81 years old presented with 7th, 9th,10th,11th, and 12th cranial nerve palsy.
Table 1.
Clinical presentation and investigations among patients with MOE.
| Patient characteristics | Number (Frequency%) |
--- |
| Otalgia | 14 (100) |
| Ear discharge | 10 (71) |
| External ear granulations | 8 (57) |
| External ear edema | 12 (85) |
| Co— existing CSOM | 3 (21) |
| Cranial nerve palsy |
| 7th nerve | 3 (21) |
| 7, 9,10,11,12th nerve | 1 (7) |
| Co-morbidities |
| Diabetes mellitus | 14 (100) |
| Hypertension | 5 (35) |
| Ischemic heart disease | 2 (14) |
| Chronic kidney disease | 1 (7) |
| Laboratory investigations |
| ESR (mm/hr) |
| <20 | 4 (29) |
| 20-40 | 6 (42) |
| >40 | 4 (29) |
| Hba1c (%) |
| < 7 (good control) | 2 (14) |
| 7–10 (poor control) | 9 (64) |
| >10 (very poor) | 3 (21) |
| Haemoglobin (g/dl) |
| <10 | 1 (7) |
| >10 | 13 (93) |
Open in a new tab
CSOM- Chronic suppurative otitis media, ESR- Erythrocyte Sedimentation Rate.
3.2. Associated co-morbidities
All patients had diabetes, and all presented with elevated blood sugar levels. Five patients had associated hypertension. One patient had hypertension, chronic kidney failure, and ischemic heart disease.
3.3. Microbiological report and laboratory investigations
Pseudomonas aeruginosa was the most common organism isolated (50%). No growth was seen in 29% cases (Fig.1.)
Fig.1.
Open in a new tab
Pie-chart depicting the organisms isolated from discharge in MOE.
Details of Erythrocyte sedimentation rate (ESR), Hb A1c and hemoglobin (Hb) at presentation has been shown in Table 1. The mean ESR was 55 mm/h, with a range of 12–88mm/hr.
Thirteen patients were diabetic with high sugar levels at presentation. Based on Hba1c, majority (64%) had poor diabetic control. Only one patient had low hemoglobin due to his chronic kidney disease.
3.4. Treatment protocol
On review of the antibiotic therapy based on the antimicrobial sensitivity report, 12 patients received monotherapy only (ceftazidime for 11, linezolid for one patient with methicillin-resistant Staphylococcus aureus (MRSA)). One patient with E-coli isolates, based on sensitivity report received a combination of Ciprofloxacin plus ceftazidime, with Klebsiella isolates received meropenem plus Ciprofloxacin. Gentamicin aural drops were used in four cases. Acetic acid ear drops (for two to three weeks) were given in all cases.
The treatment of duration varied but the mean duration observed was three weeks.
3.5. Response to treatment and follow up
After receiving treatment; eight (57%) patients had reduction in symptoms of otalgia and decrease in ear discharge within 10–14 days. They were discharged with the advice to continue acetic acid ear drops and antibiotics for one more week. They were called for follow up on week after discharge. One patient with multiple cranial nerve palsies had a hospital stay for two weeks and wanted discharge on request. He was lost to follow up. Four (29%) patients the response to treatment was poor. Hence, we did local debridement by removing the granulation tissue, necrotic tissue from the external auditory canal. Two patients improved after debridement. The pain persisted in two patients. Three patients had facial palsy with MOE, post-treatment the facial palsy completely recovered and their symptoms also improved within two weeks. One patient had persistent facial palsy after treatment.
Two patients came with other ear involvement after three months, and the affected side ear pain had subsided. Three patients came after nine months with repeat symptoms of MOE.
We could follow up six patients for 12 months. All six patient's symptoms subsided after four weeks of treatment, and for 12 months they were symptom free. ESR was done in six patients three weeks after treatment, and all showed a reduction in ESR.
4. Discussion
Malignant otitis externa is a difficult entity to treat as not only is the treatment required for a prolonged period but even the response to treatment has to be regularly monitored. Undiagnosed or partially treated MOE can progressively spread to the skull base and cause major complications such as thrombosis of lateral sinus or internal jugular vein, meningitis, Bezold's abscess and paralysis of cranial nerves (Singh et al., 2005; Nawas et al., 2013).
Similar to other studies (Courson et al., 2014; Hasibi et al., 2017), the most common presenting symptom was otalgia, which was associated with temporal and occipital headache. The presence of external auditory canal discharge, edema and granulations are all features of MOE which were present in the cases.
In our study, thirteen patients had uncontrolled diabetes. The risk of developing MOE in diabetes is more due to endarteritis, microangiopathy and small vessel obliteration (Carfrae et al., 2008).We reviewed the HbA1c status and observed that nine patients had poor control (67%).
ESR was more than 20 mm/h in 14 patients. ESR of 6 patients was repeated after three weeks, and it was noted that their ESR had come to normal. This co-related with the reduction in their symptoms and signs. This shows that ESR can be used as an adjunct to monitoring response to treatment especially in cases where repeat scan is not feasible (Rubin and Yu, 1988; Loh and Loh, 2013). HRCT temporal bone was done in all patients. Repeat HRCT was done in 4 patients after three weeks of therapy, and it showed reduced soft tissue intensity in the mastoid region. Due to non-availability of radioactive scans in our institute and the cost factor we did not do Gallium scan in our patients. Continuation of treatment was based on the response of patients to treatment and reduction of ear discharge, edema, and granulations.
Our relapse rate was 21% which is similar to other studies (Singh et al., 2005). In comparison, 2.6% was the relapse rate in another study (Hasibi et al., 2017) and in which patients who did not respond with antibacterials were switched to antifungals and they showed a favourable response.
In our series three patients (21%) presented with facial nerve palsy and two showed complete resolution of the palsy, one had persistent facial palsy. Studies have shown that facial nerve palsy is significantly less likely to improve after treatment, but the presence of cranial nerve involvement does not affect the overall prognosis (Mani et al., 2007).
Medical line of management forms the mainstay of treatment (Ridder et al., 2015). Third generation cephalosporins, intravenous ceftazidime, fluoroquinolone, carbapenems are commonly used drugs (Loh and Loh, 2013). In cases of negative culture report, studies have shown that empiric treatment with the above medication showed positive results. In our institute, we also follow the same protocol and 57% of the patients showed a favourable response within two weeks. The clinical challenge for the clinician is to decide when to stop treatment. Due to cost factor of radionuclide scan to monitor follow up, the protocol in our institution is to continue the antibiotics for a further two weeks and depending on the response of the patient further management is decided.
The limitation of our study was that the sample size was small and in patients who did not have a favorable response to treatment we did not send tissue biopsy specimens for fungal culture.
5. Conclusions
In our series, malignant otitis externa invariably presented with severe otalgia. Edema with congestion of the external auditory canal and lower cranial palsies were also seen. Diabetes as a predisposing factor was observed in all cases. Methods to evaluate complete eradication of disease should be centered on clinical symptoms and signs, but the measurement of erythrocyte sedimentation rate or radiological imaging may be used as a useful adjunct when there is uncertainty.
Declarations
Funding
No funding
Conflict of interest
No conflict of interest.
Ethical approval
Yes.
Acknowledgements
Nil.
Footnotes
Peer review under responsibility of PLA General Hospital Department of Otolaryngology Head and Neck Surgery.
Contributor Information
Saldanha Marina, Email: saldanhamarina@gmail.com.
M.K. Goutham, Email: mkgoutham565@gmail.com.
A. Rajeshwary, Email: rajeshwarisomayaji@gmail.com.
Bhat Vadisha, Email: bvadish@yahoo.co.in.
References
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11390 | https://www.vhstigers.org/ourpages/auto/2008/8/26/1219723411365/Chapter%203%20Notetaking%20Guide.pdf | • Solving Equations Using Addition and Subtraction Solve linear equations using addition and subtraction. VOCABULARY Equivalent equations Inverse operations Linear equation TRANSFORMING EQUATIONS Operation Original Equation Equivalent Equation • Add the same number to each side. x-3=5 Add x= • Subtract the same number from each side. x + 6 = 10 Subtract x= • Simplify one or both sides. x=8-3 Simplify. x= Lesson 3.1 . Algebra 1 Concepts and Skills Notetaking Guide 49 ----- ------------ ------- ---, Example 1 Add to Each Side ofan Equation You can check your solution by substituting your solution for x in the original equation. Solve x - 9 = -20 This is a subtraction equation. Use the inverse operation of addition to undo the subtraction. x - 9 = -20 Write original equation. x-9+ = -20 + Add to each side. x= Simplify both sides. Example 2 Simplify First Solve n - (-8) = -2. n - (-8) = -2 Write original equation. n + S = -2 Use subtraction rule to simplify. n+S = -2 Subtract from each side. n= Simplify both sides. o Checkpoint Solve the equation. Check your solution in the original equation. 1. x 7 = -15 2. n - (-6) = 4 . 3. -7 = 10 + Y 4. 5 - (-z) = 21 5. m - (-3) = 14 6. -S = -b + (-2) 50 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 --- -.---. - --'----. .... . ... - ------ --- ---• Solving Equations Using Multiplication and Division Solve linear equations using multiplication and division. VOCABULARY Properties of equality TRANSFORMING EQUATIONS Operation Original Equation Equivalent Equation • Multiply each side of the equation by the same nonzero number. z. , 3 2 Multiply by X= • Divide each side of the equation by the same nonzero number. 4x = 12 Divide by_ X= Example 1 Divide Each Side of an Equation Solve ax = -3. The operation is multiplication. Use the inverse operation of division to isolate the variable x. 8x = -3 Write original equation. 8x -3 0-0 Divide each side by to undo the multiplication. x = Simplify. Lesson 3.2 . Algebra 1 Concepts and Skills Notetaking Guide 51 ~------ -- --- ----- ---- ---- ------Example 2 Multiply Each Side of an Equation When you multiplyor divide both sides of an equation by a negative number, be careful with the signs of the numbers. Solve ~3 = 60. The operation is division. Use the inverse operation of multiplication to isolate the variable x. ~=60 Write original equation. -3 Multiply each side by to undo ( ~3) = (60) the division. x= Simplify. Answer The solution is o Checkpoint Solve the equation. Check your solution in the original equation. 2.6 = ~ 1.~=7 -4 7 4. -9r = -54 3.63 = 9x 52 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 Example 3 Multiply Each Side by a Reciprocal When you solve an equation with a fractional coefficient, such as 3 --m = 15 you 4 ' can isolate the variable by multiplying bythe reciprocal of the fraction. 3 Solve -"4m = 15. The fractional coefficient is -~. The reciprocal of -~ is .i. 443 3 --m = 4 15 Write original equation. ( ) (-~m) = ( Multiply each side by the reciprocal, m= Simplify. Answer The solution is PROPER'rlES OF EQUALITY Addition Property of Equality If a = b, then + c = + c. Subtraction Property of Equality If a = b, then -c = -c. . Multiplication Property of Equality If a = b, then c = c -Division Property of Equality If a = band c " 0, then o Checkpoint Solve the equation. Check your solution in the original equation. .. 5 4 5.-x = 12 6.15 = - - x 9 3 Lesson 3. 2 • Algebra 1 Concepts and Skills Notetaking Guide 53 ----• Solving Multi-Step Equations Goal Use two or more steps to solve a linear equation. Example 1 -Solve a Linear Equation Solve 2x -4 = -18. Solution To isolate the variable, undo the and then the 2x - 4 = - 18 Write original equation. Add to each side to undo the 2x -4 + = - 18 + subtraction. 2x = Simplify both sides. Divide each side by to undo the multiplication. X= Simplify. Example 2 Combine Like Terms First Solve 8x -5x + 16 = -29. Solution 8x -5x + 16 = - 29 + 16 = -29 + 16-= - 29 X= Write original equation. Combine like terms 8x and -5x. Subtract from each side to undo the addition. Simplify both sides. Divide each side by to undo the multiplication. Simplify. 54 Algebra 1 Concepts and Skills Notetaklng Guide . Chapter 3 o Checkpoint Solve the equation. Check your solution in the original equation. 2.3- 4a = 19 1.2x -5 = 9 Remember to distributethe negative sign to each term insidethe parentheses, not just the first term. 4.35 = 7y + 13y - 5 3. 12m -4m + 3 = -29 ' Example 3 Use the Distributive Property Solve 9x -5(x + 6) = -14. 9x - 5(x + 6) = -14 9x -14 -14 Write original equation. Use distributive property. Combine like terms and -14 + Add to each side to undo the subtraction. Simplify. Divide each side by multiplication. to undo the x= Simplify. Lesson 3.3 . Algebra 1 Concepts and Skills Notetaking Guide 55 Multiply by a Reciprocal First 3 Solve 24 = 4 (x + 7). 3, 24 = 4(x + 7) Write original equation. (24) = _ ( ~ )(X + 7) Multiply each side by 3 of 4' , the reciprocal = Simplify. Subtract from each side. =X Simplify both sides. o Checkpoint Solve the equation. Check your solution in the original equation. 5. -2(3 -k) = 30 6. - 38 = 4(n - 2) + 2n 7. ~(j + 23) = 8 8.12 = ~ (g + 2) 5 56 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 ,------" ,-,. ---• Solving Equations with Variables on Both Sides Solve equations that have variables on both sides. VOCABULARY Identity Example 1 Collect Variables on One Side Solve 4x - 10 = 32 - 3x. Solution look at the coefficients of the x-terms. Because 4 is greater than -3, collect the x-terms on the left side to get a positive coefficient. 4x - 10 = 32 -3x Write original equation. 4x - 10 + = 32 -3x + Add to each side. - 10 = 32 Combine like terms. - 10 + = 32 + Add to each side. = Simplify both sides. Divide each side by x = Simplify. Answer The solution is -Check 4x - 10 = 32 -3x Write original equation. 4() - 10 J: 32 - 3() Substitute for eachx. = Solution is Lesson 3.4 . Algebra 1 Concepts and Skills Notetaking GuidI'! 57 -------- --------. --- ---- Example 2 Combine Like Terms First Solve 2x - 9 + 7x = 4x - 34. 2x - 9 + 7x = 4x - 34 Write original equation. - 9 = 4x - 34 Combine like terms. - 9 -= 4x - 34 -Subtract from each side. - 9 = -34 Combine like terms. - 9 + = -34 + Add to each side. Simplify both sides. Divide each side by X= Simplify. Answer The solution is . Check this in the original equation. ., Checkpoint Solve the equation. Check your solution in the original equation. 1.6x = 5x - 33 2. 10p -22 = - P 3. 8k -22 = 10k 4. 2n -4n = 3n + 17 58 Algebra 1 Concepts and Skills Not.etaking Guide . Chapter 3 --. .---- -------------------------------Example 3 Identify Number of Solutions Solve the equation if possible. Determine whether it has one solution, no solution, or is an identity. a. 2(4x + 5) = 8x + 10 b. x - 1 = x + 7 Solution a. 2(4x + 5) = 8x + 10 Write original equation. = 8x + 10 Use distributive property. = 8x + 10-Subtract from each side. Combine like terms. Answer - - - - - - - - ,.....-- - - - - - - - - - - b. x-1=x+7 Write original equation. x-1- =x+7-Subtract from each side. Combine like terms. Answer o Checkpoint Solve the equation if possible. Determine whether the equation has one solution, no solution, or is an identity. 5. 3(x -2) = 3x -6 6. 3(x -2) = 3x + 1 Lesson 3.4 . Algebra 1. Concepts and Skills Notetaking Guide 59 ------------------ ----More on Li ear quations Goal Solve more complicated equations that have variables on both sides. STEPS FOR SOLVING LINEAR EQUATION 1 . Simplify each side by distributing and/or combining like 2. Collect variable terms on the side where the coefficient is 3. Use inverse operations to isolate the 4. Check your solution in the equation. You should simplify an equation before deciding whether to collect the variable terms on the rightside or the left side. Example 1 Solve a More Complicated Equation Solve 3(2 - x) - x = -5(x + 1). Solut ion 3(2 - x) - x = -5(x + 1) Write original equation. -x = Use distributive property. = Combine like terms. Add to each side. = Combine like terms. = Subtract from each side. x = Simplify. Answer The solution is Check 3(2 - x) - x = - 5(x + 1) Write original equation. 3(2 -) --.l -5( + 1) Substitute ---' for each x. 3( ) + J: -5( ) Simplify.
-i.
+ Multiply. Solut ion is 60 Algebra 1. Concepts and Skills Notetaking Guide . Chapter 3 ----Example 2 Solve a More Complicated Equation Solve 2{5 -4x) = 9{x + 10) -7x. 2(5 -4x) = 9(x + 10) -7x Write original equation. -7x Use distributive property. Combine like terms. mental math to add You can use Add to each side. 8x to each side of the equation. Subtract from each side. x= Divide each side by Example 3 Solve a More Complicated Equation Solve 5" (15x + 20) = 6 -2{x -4). 1 5 (15x + 20) = 6 -2(x -4) Write original equation. -- =6--- Use distributive property. Simplify. Add to each side. Subtract from each side. x= Divide each side by 1 o Checkpoint Solve the equation. Check your solution in the original equation. 1. - 6(4 - x) = 12x - 24 1 . 2. - (30 -12p) = 4 - 3(p -2) 6 Lesson 3.5 . Algebra 1 Concepts and Skills Notetaking Guide 61 ---Example 4 Compare Payment Plans Golf Course Fees A private golf course charges $1200 for membership and $5 per round played to be a member. A guest of a member pays $45 per round. Compare the costs of the members and guests. Solution Find the number of rounds for which the costs would be the same. Labels Membership fee = (dollars) Member's fee per round = (dollars) Guest's fee per round = (dollars) Number of rounds played = Algebraic 1200 + • x = • x Write linear equation. Model Subtract from each side. x= Divide each side by Answer If a member plays rounds of golf, the cost would be the same as a guest playing rounds. If a member plays more than rounds, it would cost less to be a member. If a member plays less than rounds, it would cost less to be a guest. CD Checkpoint Complete the following exercise. 3. You are looking to rent a banquet hall for a birthday party. Banquet hall A charges $200 for set-up and rental plus $15 per person. Banquet hall B charges $275 for set-up and rental plus $12 per person. Compare the costs of banquet halls A and B. 62 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 ----~- . -. _ . ---• Solving Decimal Equations Goa Find exact and approximate solutions of equations that contain decimals. VOCABULARY Rounding error Example 1 Round for the FinalAnswer Solve -28x + 31 = Solution -28x + 31 = 124 -28x = x= 124. Round to the nearest hundredth. Write original equation. Subtract from each side. Divide each side by __ When you substitute a rounded answer into the original equation, the two sides of the equation may not be exactly equal, but they should be almost equal. Use the symbol > to show that quantities are approximately equal. X z Use a calculator to get an approximate solution. X z Round to nearest hundredth. Answer The solution is approximately _ Check -28x + 31 = 124 Write original equation. -28( ) + 31 ~ 124 Substitute for x. z 124 Rounded answer is ---- Lesson 3.6 . Algebra 1 Concepts and Skills Notetaking Guide 63 ----Example 2 Solve an Equation that Contains Decimals X= Divide each side by X = Use a calculator to get an approximate solution. X = Round to nearest tenth. Answer The solution is approximately o Checkpoint Solve the equation. Round to the nearest hundredth. i.1ix 5 = 26 2.23 6y = 7 3. -48 = 13n + 14 Solve the equation. Round to the nearest tenth. 4. 6.3x - 54.8 = O.8x + 9.5 5.12.8 + 2.7x = 5.5 + 7.2x 64 Algebra 1. Concepts and Skills Notetaking Guide . Chapter 3 -----Example 3 Round for a Practical Answer Three people are equally sharing the cost of a monthly cable bill. The cable bill for this month is $41.35. What is each .person's share? Solution You can find each person's share for this month's cable bill by solving 3x = 41.35. 3x = 41.35 Write original equation. X= ----- Use a calculator to divide each side by Exact answer is a repeating decimal. x"'" -- Round to nearest cent. Answer Each person's share of the cable bill is $ Three times the rounded answer is too due to o Checkpoint Complete the following exercise. 6. Six friends are equally sharing the cost of two pizzas. The total cost of the pizzas is $18.95. What does each person owe? Lesson 3.6 . Algebra 1 Concepts and Skills Notetaking Guide 65 • Formuas Goal Solve a formula for one of its variables. V OCABULARY Formula Exa~ple 1 Solve a Temperature Conversion Formula 9 . In the formula F = -C + 32, F represents degrees Fahrenheit and 5 C represents degrees Celsius. Solve the formula for C. Solution To solve for the variable C, transform the original formula to isolate C. Use the steps for solving a linear equation. F = ~C + 32 Write original formula. 5 F -= ~C + 32 -Subtract from each side. 5 F -= ~C Simplify.
5 • (F - ) = 9 . -C 5 Multiply each side by , the reciprocal of :. (F - ) = C Simplify. Answer The new formula is C = (F - ). 66 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 -------- - ------ ----Example 2 Solve and Use an Area Formula The formula for the area of a rectangle is A = £w. a. Find a formula for width w in terms of area A and length l, b. Use the new formula to find the width of a rectangle that has an area of 54 square inches and a length of 9 inches. Solution a. Solve for width w. A = £w Write original formula. =w Divide each side by b. Substitute the given values into the new formula. w = inches Example 3 Solve and Use a Density Formula The density d of a substance is found by dividing its mass m by its volume v. a. Solve the density formula d = m for volume v. v b. Use the new formula to find the volume of a substance that has a density of 7.2 grams per cubic centimeter and a mass of 25.2 grams. Solution a. Solve for volume v. d = m Write original formula. v d =m Multiply each side by _ Divide each side by b. Substitute the given values into the new formula. cubic centimeters Lesson 3.7 . Algebra 1 Concepts and Skills Notetaking Guide 67 ----Solve and Use a Distance Formula The distance traveled d is found by multiplying the rate (or speed) r by the time t. a. Solve the distance formula d = rt for time t. b. A car travels 1770 miles on a highway at an average speed of 59 miles per hour. How long does the trip take? Solution a. d = rt Write original formula. Divide each side by = t Simplify. b. t = Answer The trip takes o Checkpoint Complete the following exercises. 1. The perimeter P of a rectangle with length £ and width w is P = 2£ + 2w. Solve the equation for .E. 2. The volume Vof a box with length .E, width w, and height h is V = twn. Solve the equation for w. 3. Use the result from Exercise 2 to find the width w of a box with a length of 2 feet, a height of 3 feet, and a volume of 12 cubic feet. 68 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 --------atios and Rates Goal Use ratios and rates to solve real-life problems. VOCABULARY Ratio of a to b Rate of a per b Unit rate Unit analysis A ratio compares two quantities measured in the same unit. The ratio itself has no units. A rate compares two quantities that have different units. Example 1 Find a Ratio A baseball player has 16 hits in 44 at bats. Find the ratio of hits to at bats. hits Ratio = at bats Answer The ratio is , which is read as " to " Find a Unit Rate A car travels 330 miles in 6 hours. What is the average speed of the car in miles per hour? 3300 Rate = = 6 0 Answer The average speed of the car is Lesson 3.8 . Algebra 1 Concepts and Skills Notetaking Guide 69 -------- ------o Checkpoint Complete the following exercises. 1. Your team won 8 out of 2. A horse can travel 48 miles 12 softball games, with in 4 hours. Find the average no tie games. What was speed of the horse in miles the team's ratio of wins per hour. to losses? Example 3 Use UnitAnalysis Use unit analysis to convert 6 minutes to seconds. Solution Use the fact that 60 = 1 = 1.
50'11 1 60 1 I 6 __ • -1---r=\=I_~~::~1 Answer 6 minutes equals Example 4 Use a Rate The average mileage for your car is 34 miles per gallon of gasoline. How many miles can you drive on a full 14 gallon tank of gasoline? Solution distance = (34 }14 __) Substitute rate and gallons. = (34)(14) Answer You can drive about ---- Use unit analysis. Multiply. on 14 gallons. 70 Algebra 1 Concepts and Skills Notetaklng Guide . Chapter 3 --- -----------Example 5 Apply UnitAnalysis I ! ~ I i I ~ I i t I t I I . I , I I I I I I Exchanging Money You are visiting Finland and you want to exchange $350 for euros. The rate of currency exchange is 0.92 euro per United States dollar when you exchange the money. How many euros will you receive? Solution You can use unit analysis to write an equation to convert dollars into euros. 0.92 1 1[ E = (350 __)(-O·1 -----r=9 1~1~IF'--I) Write equation. E = (350)(0.92 __) Use unit analysis. E= ---- Multiply. Answer You will receive ---- o Checkpoint Complete the following exercises. 3. Use unit analysis to convert 3 years to days. 4. A lawnmower can mow about 1.25 acres per gallon of fuel. How many acres are mowed after using 6 gallons of fuel? 5. In Example 5, you have 34 euros when you leave Finland. The rate of currency exchange is now 0.93 euros per United States dollar. How many United States dollars will you get back? Round to the nearest cent. Lesson 3.8 • Algebra 1. Concepts and Skills Notetaking Guide 71 ercents Goal Solve percent problems. VOCABULARY Percent Base number THREE TYPES OF PERCENT PROBLEMS Question Given Need to Find What is p percent of b? a is p percent of what? a is what percent of b? Example 1 Number Compared to Base is Unknown In the verbal What is 40% of 60 inches?
model, the number a is compared to the base number b. Verbal o = Ip percent I·0 Model Labels Number compared to base = a (inches) Percent = 40% = (no units) Base number = (Inches) Algebraic a = (__)() = Model Answer is 40% of 60 inches. 72 Algebra 1. Concepts and Skills Notetaking Guide . Chapter 3 ------------~---- --..-. -----Example 2 Base Number is Unknown Twelve dollars is 15% of what amount of money? Verbal o = Ip percent I. 0 Model Labels Number compared to base = (dollars) Percent = 15% = (no units) Base number = b (dollars) Algebraic __ = ( __ ) b Model =b Answer $12 is 15% of Example 3 Percent is Unknown Two hundred fifty-five is what percent of 85? Verbal o = Ip percent I· 0 Model Labels Number compared to base = (no units) Percent = p% = - p-(no units) 100 Base number = (no units) Algebraic -- = (160)(-) Model =~ 100 .e. 100 =p Answer 255 is of 85. Lesson 3.9 ' Algebra 1 Concepts and Skills Notetaking Guide 73 o Checkpoint Complete the following exercises. 1. What is 65% of $220? 2. 46.5 is 30% of what number? 3~ One hundred ninety-six is what percent of 140? The discount is the regular price minus the sale price. Example 4 Model and Use Percents Discount Percent A store sells a television for $350. A week later the same model is on sale for $297.50. What is the discount percent? Verbal I Discount I= I p percent I·IRegular price I Model Discount = (dollars) Percent = p% = -p (no units) 100 Regular price = (dollars) -p ( Algebraic --- 100 Model =-p --100 p= Answer The discount percent is __ 74 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 .-- - - .--- - - - _ ._- Words to Review Give an example of the vocabulary word. Equivalent equations Inverse operations Linear equation , Properties of equality Identity Rounding error Formula Ratio of a to b Rate of a per b Unit rate Words to Review . Algebra 1 Concepts and Skills Notetaking Guide 75 Unit analysis Percent Base number Review your notes and Chapter 3 by using the Chapter Review on pages 189-192 of your textbook. 76 Algebra 1 Concepts and Skills Notetaking Guide . Chapter 3 |
11391 | https://www.youtube.com/watch?v=ot075b_LLHg | Transcription Termination in Prokaryotes
Hussain Biology
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Posted: 29 Apr 2019
Two classes of transcription terminators, Rho-dependent and Rho-independent, have been identified throughout prokaryotic genomes. These widely distributed sequences are responsible for triggering the end of transcription upon normal completion of gene or operon transcription, mediating early termination of transcripts as a means of regulation such as that observed in transcriptional attenuation, and to ensure the termination of runaway transcriptional complexes that manage to escape earlier terminators by chance, which prevents unnecessary energy expenditure for the cell.
Rho-dependent terminators
Rho-dependent transcription terminators require a protein called Rho factor, which exhibits RNA helicase activity, to disrupt the mRNA-DNA-RNA polymerase transcriptional complex. Rho-dependent terminators are found in bacteria and phage. The Rho-dependent terminator occurs downstream of translational stop codons and consists of an unstructured, cytosine-rich sequence on the mRNA known as a Rho utilization site (rut) for which a consensus sequence has not been identified, and a downstream transcription stop point (tsp). The rut serves as a mRNA loading site and as an activator for Rho; activation enables Rho to efficiently hydrolyze ATP and translocate down the mRNA while it maintains contact with the rut site. Rho is able to catch up with the RNA polymerase, which is stalled at the downstream tsp sites. Contact between Rho and the RNA polymerase complex stimulates dissociation of the transcriptional complex through a mechanism involving allosteric effects of Rho on RNA polymerase.
Rho Dependent
Intrinsic transcription terminators or Rho-independent terminators require the formation of a self-annealing hairpin structure on the elongating transcript, which results in the disruption of the mRNA-DNA-RNA polymerase ternary complex. The terminator sequence in DNA contains a 20 basepair GC-rich region of dyad symmetry followed by a short poly-T tract or "T stretch" which is transcribed to form the terminating hairpin and a 7–9 nucleotide "U tract" respectively.
The hairpin formation causes RNA polymerase stalling and destabilisation, leading to a greater likelihood that dissociation of the complex will occur at that location due to an increased time spent paused at that site and reduced stability of the complex.
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Transcript:
Oh in the series of videos we have been discussing about the transcription in prokaryotes and now in this video we'll be discussing about the termination of transcription in prokaryotes the termination of transcription in e.coli or in prokaryotes proceeds in two ways either it's row independent termination or it's row dependent termination row here is the protein that means in one case there is no involvement of pro protein well as in other case there is involvement of pro protein in row independent termination the physical modified structure of RNA transcript terminates the transcription whereas in case of row dependent termination the helices protein row protein terminates the transcription the second point we see here is that in row independent termination the hairpin loop like structure pulls off RNA transcript from there RNA polymerase complex thereby terminating the transcription as you can see in this diagram the hairpin loop like structure comes into action in row independent termination now looking at the Road appendant termination the helicase protein which is the hexameric protein has structure like this it binds to the right side on RNA transcript and gets to the polymerase enzyme where it terminates the transcription and this row protein is ATP dependent protein now let's discuss a row independent termination in detail first in this diagram we can see we have the DNA molecule having RNA polymerase attach it to it this RNA polymerase enzyme works on the lower strand that's the template strain and we had this RNA molecule being synthesized it here and here in this diagram we can see we had the termination site here having a poly ATP or editing and timing peers to see how he open loop homes we see in the next step the RNA molecule which is getting synthesized it has got couple of GC regions like GC g GC c g so what happens with these GC rich regions is that the GC bases peers with each other and form the hairpin loop like structure shown in the diagram actually this lupone's due to palindromic sequences on RNA transcript here in this diagram it is these two regions which come together and poms loop now this loop reduces the length of rna-dna hybrid so from this structure the RNA will get a physical traction but to pull out RNA molecule from the polymerase machinery it needs a weak link we should break easily and this is provided by a tear each reagent DNA white template strand having poly I'd mean and transcribes poly us all in the RNA chain so this region au base pair is the weak point where from the transcription is terminated easily when the hairpin loop like structure forms and in the end we get RNA molecule out of the polymerase complex easily as shown in the diagram so this is how ro independent termination works now let's see how ro dependent termination is drawn in this diagram we have DNA molecule having RNA polymerase attached a trait which has synthesized RNA molecule as shown in the diagram this nascent RNA molecule has one interesting site on it called the rut site ROH utilization site to this rut site the ro helices protein binds and starts moon towards the transcription machinery RNA polymerase as shown in the animation and it must be noted that this hill case uses energy from the ATP hydrolysis when this helices reaches the end of RNA molecule it encounters that DNA RNA duplex and this being the helicase enzyme unwinds the duplex easily and finally our net transcript is released from the complex this way ro dependent termination is driven in the e.coli so this is all about termination of transcription in prokaryotes I hope you liked the video if you liked it give it a thumbs up do consider supporting my work on patreon and also make sure subscribe this channel Thanks |
11392 | https://mcckc.edu/tutoring/docs/blue-river/math/functions/Simplifying_Rational_Expressions.pdf | Rational Expressions A quotient of two integers, , where 0, is called a rational expression. Some examples of rational expressions are , , , and . When 4, the denominator of the expression becomes 0 and the expression is meaningless. Mathematicians state this fact by saying that the expression is undefined when 4. One can see that the value , makes the expression undefined. On the other hand, when any real number is substituted into the expression , the answer is always a real number. There are no values for which this expression is undefined. EXAMPLE Determine the value or values of the variable for which the rational expression is defined. a) b) Solution a) Determine the value or values of x that make 2x – 5 equal to 0 and exclude these. This can be done by setting 2x – 5 equal to 0 and solving the equation for x. 2 5 0 2 5 Do not consider when considering the rational expression . This expression is defined for all real numbers except . Sometimes to shorten the answer it is written as . b) To determine the value or values that are excluded, set the denominator equal to zero and solve the equation for the variable. 6 7 0 7 1 0 7 0 or 1 0 7 1 Therefore, do not consider the values 7 or 1 when considering the rational expression . Both 7 and 1make the denominator zero. This is defined for all real numbers except 7 and 1. Thus, 7 and 1. SIGNS OF A FRACTION Notice: Generally, a fraction is not written with a negative denominator. For example, the expression would be written as either or . The expression can be written since 4 4 or 4. Other examples of equivalent fractions: " " " " " " # # # # # # SIMPLIFYING RATIONAL EXPRESSIONS A rational expression is simplified or reduced to its lowest terms when the numerator and denominator have no common factors other than 1. The fraction is not simplified because 9 and 12 both contain the common factor 3. When the 3 is factored out, the simplified fraction is . $ · $ · The rational expression is not simplified because both the numerator and denominator have a common factor, b. to simplify this expression, factor b from each term in the numerator, then divide it out. Thus, becomes when simplified. To Simplify Rational Expressions 1. Factor both the numerator and denominator as completely as possible. 2. Divide out any factors common to both the numerator and denominator. Example 1 Simplify Solution Factor the greatest common factor, 5, from each term in the numerator. Since 5 is a factor common to both the numerator and denominator, divide it out. & ' · Example 2 Simplify Solution Factor the numerator; then divide out the common factor. 1 Example 3 Simplify Solution Factor the numerator; then divide out common factors. = 4 Example 4 Simplify Solution Factor both the numerator and denominator, then divide out common factors. Example 5 Simplify ( ( ( ( Solution Factor both the numerator and denominator, then divide out common factors. ( ( ( ( ( ( ( ( ( ( Example 6 Simplify Solution Factor both the numerator and denominator, then divide out common factors. & ' Example 7 Simplify Solution Factor both numerator and denominator, then divide out common factors. &' Consider the expression , a common student error is to attempt to cancel the x or the 3 or both x and 3 appearing in this expression. This is WRONG! $ $ $ $ does not equal 2 It is WRONG because factors are not being reduced. Evaluating this expression for an easy value, such as 1, would show that the illustrated cancellations are WRONG. If 1, becomes . Remember: Only common factors can be divided out from expressions. 5 In the denominator of the example on the left, 4, the 4 and x are factors since they are multiplied together. The 4 and the x are also both factors of the numerator 20, since 20 can be written 4 · · 5 · . Some students incorrectly divide out terms. In the expression , the x and –4 are terms of the denominator, not factors, and therefore cannot be divided out. Recall that when -1 is factored from a polynomial, the sign of each term in the polynomial changes. EXAMPLES: 3 5 13 5 3 5 6 2 16 2 2 6 Example 8 Simplify Solution Since each term in the numerator differs only in sign from its like term in the denominator, factor-1 from each term in the denominator. 1 Example 9 Simplify Solution 4 1 ADDITIONAL EXERCISES Determine the value or values of the variables for which the expression is defined. 1. 2. 3. 4.
+ 5. + 6. Simplify 7. ,,-
, 8. ../ +. 9. ,,-, 10. +
11. 12. 13. 14.
15. 0 0 16. 17. 1+ 1 18. 19. + 20. Answers 1. 3, 4 2. 3. 6, 1 4. 0, 5. 6, 2 6. , 0 7. - 8. / + 9. - 10. 3 11. 2 12. – 7 13. – 2 14. 15. 0 16. 17. 1+ 18. – 7 19. 20. – |
11393 | https://medium.com/algorithm-and-datastructure/longest-arithmetic-subsequence-of-given-difference-f49fa8440904 | Longest Arithmetic Subsequence of Given Difference | by Omar Faroque | Algorithm and DataStructure | Medium
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Longest Arithmetic Subsequence of Given Difference
Omar Faroque
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Given an integer array arr and an integer difference, return the length of the longest subsequence in arr which is an arithmetic sequence such that the difference between adjacent elements in the subsequence equals difference.
Example 1:
Input: arr = [1,2,3,4], difference = 1
Output: 4
Explanation:The longest arithmetic subsequence is [1,2,3,4].
Example 2:
Input: arr = [1,3,5,7], difference = 1
Output: 1
Explanation:The longest arithmetic subsequence is any single element.
Example 3:
Input: arr = [1,5,7,8,5,3,4,2,1], difference = -2
Output: 4
Explanation:The longest arithmetic subsequence is [7,5,3,1].
Constraints:
1 <= arr.length <= 10^5
-10^4 <= arr[i], difference <= 10^4
Solution:
Basically, we have to found sequence with the difference between neighbours is ‘difference’
We have to iterate over all the numbers and find the second number to make a pair with the difference is ‘difference’.
a[I]-a[j]=difference
a[I]-difference=a[j]
We can keep a[i] in the map with value 1 by default.
But if we find the element a[j] in the map, we have to put the value a[I]=a[j]+1
Now look at the java implementation,
public class…
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11394 | https://medium.com/@Brain_Boost/linear-algebra-the-determinant-f4db192918cd | Linear Algebra: The Determinant. Some linear transformations stretch out… | by Brain_Boost | Medium
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Linear Algebra: The Determinant
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Some linear transformations stretch out space while others squish it. But, exactly how much are things stretched and squished? More specifically to measure the factor by which, the area of a given region increases or decreases. For example lets look at the matrix with the columns 3,0 and 0,2.
source-
It scales ihat by a factor of 3 and scales jhat by a factor of 2. Now lets go back and focus our attention on the one by one square whose bottom sits on ihat and whose left side sits on jhat. After the transformation this turns into a 2 by 3 rectangle. Since this region started with area 1 but ended up with area 6 we can say that the linear transformation has scaled the area by a factor of 6.
Now lets compare that to a matrix with the columns 1,0 and 1,1. Which means that ihat stays in place and jhat moves over to 1,1.
source-
That same unit square determined by ihat and jhat now has become slanted and turned into a parallelogram but its area is still 1(its base and height both have the length of 1). So even though this transformation smushes things it still leaves areas unchanged.
Though if you know how much of that single unit square changes, it can tell you how any region in space changes in terms of area. Whatever happens to one square in the grid has to happen to the other squares in the grid no matter the size(grid lines remain parallel and evenly spaced). Then any shape that is not a grid square can be approximated by grid squares pretty well(if you use small enough grid squares). Since the area of those grid squares are being scaled by that amount so is any shape that you want to figure out how much the area has changed.
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This scaling factor by which is linear transformation changes an area is known as the determinant of the transformation. The determinant of a region would be 3 if the linear transformation increases the area by a factor of 3. The determinant of a 2d transformation is 0 if it squishes all of space on to a line or single point.
Though its important to note that the full concept of the determinant allows for negative values. But what would that even mean? Well it has to do with the idea of orientation. Another way to think about it is in terms of ihat and jhat. In their starting positions jhat is to the left of ihat. If after a transformation jhat is now on the right of ihat the orientation of space has been inverted(negative determinant and the absolute value is still the scaling factor).
Though why do negative determinants means orientation flipping? Well as ihat gets closer to jhat in the transformations the determinant gets smaller and smaller. Then at 0 they are on top of each other so logically for a negative determinant their positions must be inverted.
Now what about for 3d? Well in 3d the determinant also tells you how much the volume gets scaled. In 3d the three basis vectors form a cube and through linear transformations the cube gets stretched out and squished in a parallelepiped. The cube starts with a volume of 1 and the determinant gives the value of how the volume is scaled, so one can think of the determinant as the volume of the parallelepiped.
A determinant of 0 would mean all of space is squished into something with 0 volume(a flat plane, line, point). What do negative determinants mean for 3d? It has a similar meaning in terms of orientation, it means that the positions of ihat and jhat are reversed.
Finally, how do you compute the determinant? Lets take a look at a 2 by 2 matrix with the entries a, b, c and d.
Press enter or click to view image in full size
source-
This leaves us with the question, where does this formula come from? Lets say that b and c are both 0. Then the term a tells you how much ihat is stretched in the x direction and the term d tells you how much jhat is stretched in the y direction. So since the other terms are 0 it makes sense that a times d gives us the area of the rectangle. Even if only one of b or c are 0 you will have a parallelogram with a base a and a height of d. If b and c are both non 0 then the b times c term tells you how much the parallelogram is stretched or squished in the diagonal direction.
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May 2, 2024
Individually, the elements of the matrix do different things, but when we combine them, as we do here with multiplication: 3 x 2 = 6, we kind of eliminate the individual effect and like an engineering truss, "they" move as one.
Correct/incorrect/both/neither?
--
1 reply
Reply
Dida Koul
Apr 15, 2024
Great article. Would also benefit from a determinant example in 3d
--
Reply
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Anna C. Ganster, MD, Mohamed Farooq Ahamed, MD, FAAP, Mamta Fuloria, MD, FAAP, 2016. "Surgical Emergencies of the Chest and Abdomen in the Newborn", American Academy of Pediatrics Textbook of Pediatric Care, Thomas K. McInerny, MD, FAAP, Henry M. Adam, MD, FAAP, Deborah E. Campbell, MD, FAAP, Thomas G. DeWitt, MD, FAAP, Jane Meschan Foy, MD, FAAP, Deepak M. Kamat, MD, PhD, FAAP, Rebecca Baum, MD, FAAP, Kelly J. Kelleher, MD, MPH, FAAP
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Updated on September 29, 2020
Newborns often present with nonspecific gastrointestinal (GI) signs and symptoms, indicating either a primary GI pathology or other conditions (most notably, infections). Thus, an understanding of the common presenting GI signs and symptoms, their differential diagnoses, and the diagnostic workup and management is essential in the care of neonates. Although this chapter primarily focuses on GI pathologies that require urgent interventions, choanal atresia (CA) and neck masses in the newborn period are briefly discussed as well.
Most neonates with GI pathology present within the first few days after birth; thus, the postnatal history may not...
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11396 | https://study.com/skill/learn/how-to-find-local-extrema-by-checking-critical-points-of-a-function-explanation.html | How to Find Local Extrema by Checking Critical Points of a Function | Calculus | Study.com
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How to Find Local Extrema by Checking Critical Points of a Function
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00:04 How to find local…
04:41 How to find local…
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Example SolutionsPractice Questions
Steps for Finding Local Extrema by Checking Critical Points of a Function
Step 1: Find the critical points of f(x) by equating the first derivative to zero.
Step 2: Use the intervals between critical points to evaluate if f′(x) is positive or negative in that interval. This can be done by selecting x values in the interval and substituting into f′(x). Note that we only care about the sign of the answer, not the value itself. For example if f′(1)=−3, then we only need to extract that the derivative is negative (−) at x=1.
Step 3: Determine any critical points where the derivative changes sign as local extrema. Be sure to exclude any values x not in the domain of f.
Changing from negative (−) to positive (+) means f(x) has a local minimum.
Changing from positive (+) to negative (−) means f(x) has a local maximum.
Definitions for Finding Local Extrema by Checking Critical Points of a Function
Critical Point: A value x such that f′(x)=0 or f′(x) fails to exist.
Local Extrema: A point on the function f that is either a maximum or minimum point for nearby values of x.
Increasing/Decreasing: A special relationship between f′(x) and f(x) exists in that the sign of the derivative tells us if the function is increasing or decreasing at that value of x.
If f′(x)<0 (negative) then the function is decreasing.
if f′(x)>0 (positive) then the function is increasing.
Now let's practice two examples of finding local extrema by checking critical points of a function.
Example Problem 1: Finding Local Extrema by Checking Critical Points of a Function
Use the critical points of the function to determine all of the local extrema of the function f(x)=7 x 2+21 x−4.
Step 1: Find the critical points of f(x).
To do this, we find f′(x) and determine where f′(x)=0 and any x where f′(x) does not exist.
Taking the derivative of f we get
d d x[7 x 2+21 x−4]=14 x+21.
Since we have a polynomial, there are no such x that make f′(x) undefined. Setting f′(x)=0 and solving we get
14 x+21=0 14 x=−−21 14 x=−3 2 This is our only critical point of f.
Step 2: Use the intervals between critical points to evaluate if f′(x) is positive or negative in that interval.
Since the only critical point is x=−3 2 we split the real numbers up into to intervals, (−∞,−3 2) and (−3 2,∞).
Now we select a test value in each interval. The values of x=−2 and x=0 work for their respective intervals. Evaluating these points in f′(x) we get
f′(−2)=14(−2)+21=−28+21=−7 and we have f′(x) is negative (−) on the interval (−∞,−3 2).
f′(0)=14(0)+21=0+21=21 and we have that f′(x) is positive (+) on the interval (−3 2,∞).
Step 3: Determine any critical points where the derivative changes sign as local extrema. Be sure to exclude any values x not in the domain of f.
We have that the derivative changes sign at x=−3 2, it goes from negative (−) to positive (+). This means that the function goes from decreasing to increasing x=−3 2.
Thus we have a local minimum at x=−3 2.
Example Problem 2: Finding Local Extrema by Checking Critical Points of a Function
Use the critical points of the function to determine all of the local extrema of the function f(x)=4 x+4 x 2.
Step 1: Find the critical points of f(x).
To do this, we find f′(x) and determine where f′(x)=0 and any x where f′(x) does not exist.
Taking the derivative of f using quotient rule we get
d d x[4 x+4 x 2]=4(x 2)−(4 x+4)(2 x)(x 2)2=4 x 2−8 x 2−8 x x 4=−4 x 2−8 x x 4
Since we x 4 in the denominator, the value of x=0 will make f′(x) undefined. Now, setting f′(x)=0 and solving we get
−4 x 2−8 x x 4=0−4 x 2−8 x=0(Multiply both sides by x 4)−x(4 x+8)=0(Factored the expression on the left side). Separating these and solving we get x=0 which was already a point at which f′(x) is undefined, and x=−2. Thus we have the critical points x=−2 and x=0.
Step 2: Use the intervals between critical points to evaluate if f′(x) is positive or negative in that interval.
Here we split the real numbers up into to intervals, (−∞,−2), (−2,0) and (0,∞).
Now we select a test value in each interval. The values of x=−3, x=−1 and x=1 work for their respective intervals. We can simplify the derivative expression to −x(4 x+8) for the purpose of evaluating where f′(x)=0. Then evaluating these points we get
f′(−3)=−(−3)(4(−3)+8)=3(−12+8)=(+)(−)=(−). Note that we only care about the sign and not the value, thus we get that f′(x) is negative (−) on the interval (−∞,−2).
f′(−1)=−(−1)(4(−1)+8)=1(−4+8)=(+)(+)=(+). Note that we only care about the sign and not the value, thus we get that f′(x) is positive (+) on the interval (−2,0).
f(1)=−(1)(4(1)+8)=−1(4+8)=(−)(+)=(−). Note that we only care about the sign and not the value, thus we get that f′(x) is positive (−) on the interval (0,∞).
Step 3: Determine any critical points where the derivative changes sign as local extrema. Be sure to exclude any values x not in the domain of f.
We have that the derivative changes sign at every critical point of f. It goes from negative to positive and back to negative. However, x=0 is not in the domain of f and thus cannot be a local extrema. This means the only local extrema is x=−2 and since the function goes from decreasing to increasing it is a local minimum.
Thus we have a local minimum at x=−2.
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Table of Contents
Steps for Finding Local Extrema by Checking Critical Points of a Function
Definitions for Finding Local Extrema by Checking Critical Points of a Function
Example Problem 1
Example Problem 2
Test your current knowledge
Practice
Finding Local Extrema by Checking Critical Points of a Function
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11397 | https://www.geeksforgeeks.org/maths/irregular-polygon/ | Irregular Polygon
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Irregular Polygons are polygons that don't have all their sides equal. All the angles are not of equal measure in irregular polygons. Some examples of irregular polygons include the right triangle, isosceles triangle, scalene triangle, rectangle and many more.
In this article, we will explore irregular polygons, properties of irregular polygons, types of irregular polygons and irregular polygon formulas. We will also discuss the difference between regular and irregular polygons and solve some examples related to irregular polygons. Let's start our learning on the topic "Irregular Polygons ".
Table of Content
Definition of Irregular Polygons
Properties of Irregular Polygons
Types of Irregular Polygons
Difference Between Irregular and Regular Polygons
Irregular Polygons Formulas
Examples on Irregular Polygons
Irregular Polygons Definition
A polygon is said to be an irregular polygon when all the sides and angles of the polygon are unequal. In other words, the polygon with all its sides and angles of different measures is called an irregular polygon. All the polygons with unequal sides and angles come under irregular polygons. Some irregular polygon examples are right triangle, isosceles triangle, scalene triangle, rectangle, irregular pentagon, irregular hexagon etc.
Properties of Irregular Polygons
Some of the properties of irregular polygons are:
The sides of the irregular polygons are unequal.
The angles of the irregular polygons are unequal.
Some examples of irregular polygons include rectangles, parallelograms, trapezium, right triangles, obtuse triangles and many other polygons whose sides and angles are not equal.
Examples of Irregular Polygons
There are various different examples of irregular polygons including scalene triangles, isosceles triangles, right triangles, rectangles, irregular pentagons, irregular hexahexagon many more.
Scalene Triangle
Triangle in which all the three sides are different is called as scalene triangle.
Some Formulas of Scalene Triangle
Below are some formulas related to scalene triangle.
Area of scalene triangle is given by Heron's formula.
Area = √[s (s-a) (s-b) (s-c)]
where,
a, b and c are sides of scalene triangle
s = (a + b + c) /2
Perimeter of Scalene Triangle = Sum of All Three Sides.
Isosceles Triangle
Triangle in which two sides are equal is called as isosceles triangle.
Some Formulas of Isosceles Triangle
Below are some formulas related to isosceles triangle.
Height of isosceles triangle = √[(a2 - b2)/4]
Area of isosceles triangle = (1/2) × base × height
Perimeter of isosceles triangle = sum of all three sides
Right Triangle
Triangle with one of its angles as right angle is called right triangle.
Some Formulas of Right Triangle
Below are some formulas related to right triangle.
Area of Right triangle = (1/2) × base × height
Perimeter of Right triangle = Base + Perpendicular + Hypotenuse
Pythagoras theorem: (Hypotenuse)2 = (Base)2 + (Perpendicular)2
Rectangle
Quadrilateral whose all angles and opposite sides are equal is called as rectangle.
The four sides of rectangle include two length and two breadths. The measure of length and breadth can be equal and unequal.
Some Formulas of Rectangle
Below are some formulas related to rectangle.
Area of the rectangle = length × breadth
Perimeter of rectangle = 2(length + breadth)
Irregular Pentagon
Pentagon whose sides are not equal is called as the irregular pentagon.
Irregular Hexagon
Hexagon whose sides are not equal is called as irregular hexagon.
Difference Between Irregular and Regular Polygons
Below table gives the difference between the irregular and regular polygons.
| Characteristics | Regular Polygons | Irregular Polygons |
---
| Definition | The polygon with equal sides and angles is called regular polygons. | The polygon with unequal sides and angles is called irregular polygon. |
| Examples | Some examples of regular polygon include square, equilateral triangle etc. | Some examples of irregular polygon include rectangle, scalene triangle etc. |
| Measure of Sides | All sides of the polygon are equal. | All the sides of the polygon are unequal. |
| Measure of Angles | All angles of the polygon are equal. | All angles of the polygon are not equal. |
Irregular Polygons Formulas
Different formulas of the irregular polygon like area of irregular polygon, perimeter of irregular polygon, sum of interior angle of irregular polygons, sum of exterior angles of irregular polygons are given below.
Area of Irregular Polygons
Area of irregular polygons can be determined by dividing the irregular polygon in some parts that gives regular polygons. After dividing the irregular polygons in regular parts, we find the area of these regular parts. After finding the areas we add all the areas to determine the area of irregular polygon.
Perimeter of Irregular Polygons
Perimeter of irregular polygons is obtained by adding all the lengths of all the sides of the irregular polygon.
Perimeter of Irregular Polygon = Sum of all Sides of Irregular Polygon
Sum of Interior Angles of Irregular Polygons
Sum of interior angles of irregular polygon is obtained by subtracting 2 from number of sides of irregular polygon and then multiplying the resultant by 180°. The formula for the sum of interior angles of the irregular polygon is same as the formula for the sum of interior angles of regular polygon.
Sum of interior angles of irregular polygon = (n - 2) × 180°
Sum of Exterior Angles in Irregular Polygons
Sum of exterior angles in irregular polygon is equal to 360°. It is same as the sum of exterior angles of the regular polygons.
Sum of exterior angles in irregular polygon = 360°
Read More,
Polygon
Types of Polygon
Diagonals
Polygon Formula
Examples on Irregular Polygons
Example 1: Find the perimeter of the rectangle with length 12 cm and breadth 5 cm.
Solution:
Area of Rectangle = length × breadth
Area of Rectangle = 12 × 5
Area of Rectangle = 60 cm2
Example 2: Find the sum of interior angles of irregular polygon with 15 sides.
Solution:
Sum of interior angles of irregular polygon = (n - 2) × 180°
Sum of interior angles of irregular polygon with 15 sides = (15 - 2) × 180°
Sum of interior angles of irregular polygon with 15 sides = 13 × 180°
Sum of interior angles of irregular polygon with 15 sides = 2340°
Example 3: Find the area of the right- triangle with base 12 cm and height 5 cm.
Solution:
Area of Right Triangle = (1/2) × base × height
Area of Right Triangle = (1/2) × 12 × 5
Area of Right Triangle = 30 cm2
Practice Questions on Irregular Polygons
Q1: Find the area of the scalene triangle with sides 10cm, 20 cm and 17 cm.
Q2: Find the sum of interior angles of irregular polygon with 10-sides.
Q3: Find the perimeter of the irregular hexagon with sides 10 units, 2 units, 13 units, 9 units, 15 units and 5 units.
Q4: Find the area of rectangle with length and breadth 9 cm and 4 cm respectively.
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11398 | https://www.youtube.com/watch?v=Q7-PHHa5x-c | Probability of License Plates
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A simple Probability License Plate problem
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Transcript:
all right this is a continuation on probability let's talk about what's the probability of getting a license plate that has this so what's the probability of actually getting this license plate well we'll assume that the first three spaces will always be letters so there'll be a b c and so on and while assume the last three will always be digits so it'll be zero one two all the way to nine nine of course that's Z so what's the probability of getting this particular plate all right so if the first three can only be letters we need to find the probability probability of getting a g first and then need to find the probability of getting the second letter be a g so then we got to find the probability of the second letter to be a g whoops G then the next letter the probability of it being a g as well then we need to find the probability of the of the next part being being a six so what's the probability of getting a six and then the probability of getting a nine and finally the probability of getting a three probability of getting a three so how what's the probability of getting G as the first letter well that's one letter out of a total of 26 letters so the probability of getting a g in the first space space is 1 out of 26 and that's true for the next one g 1 out of 26 again getting a g is 1 out 26 chance now what's the probability of getting a six well that's one number out of a total of 10 10 so we have zero through nine so there are 10 digits so there's there's we want this one digit out of possible 10 digits and then we do the same for the nine so that's out of 10 and the same for the last one that's out of 10 as well well now there's actually a much simpler way of doing this this is one this is one thing that we want of out of all the possible different types of plates so we have an actual we have actually 26 26 26 10 10 10 will give us a total number of plates possible so if we did a little bit of math we could find out the total number of plates possible so that's 2 6 26 26 10 10 10 that is equal to that's a really big number that is equal to whoops see uh, 17.5 million 17.5 million so put a bunch of zeros so really the probability getting this one plate is one is one out of the 17.5 million million so it is really unlikely to get this plate out of anyone let's find the probability of getting one so let's say we want a license plate that was that was a b c 1 2 three what's the probability of that well getting an a is one out of 26 getting a b is one out of 26 and getting a c is one out of 26 and getting a one is 1 out of 10 getting a two is one out of 10 and getting a three is one out of is one out of 10 10 so this probability is again one out of the 17 mil or a million 17.5 million so getting this one is really remote extremely remote now let's say that they side to make it where license plates cannot repeat letters so this can't be G and this can't be g once this is a g so this has to be a different letter the first letter can be any of the 26 letters 26 letters the next one can only be 25 of the 26 letters and the reason this is 25 is because we can't repeat the first letter then the next one must be 24 and that's because we can't repeat these two first letters then we have then we have a digit so it could be any of the 10 digits and the next one can only be nine of the 10 digits because if we had 10 out of 10 we'd be repeating again and finally we'd have eight so let's find out the total number of PL of of of plates possible so we have 26 25 24 24 10 9 8 that is equal to 11 million so that's equal to 11 million so once you unable to repeat letters you lose around 6 million 6 million plates so if you're in a big state like California 11 million plates is kind of pushing it so you want to have as many plates as possible so you'll allow you'll allow the letters to repeat |
11399 | https://emedicine.medscape.com/article/206490-differential | Beta Thalassemia Differential Diagnoses
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Tools & Reference>Hematology
Beta Thalassemia Differential Diagnoses
Updated: Jan 26, 2024
Author: Pooja Advani, MD; Chief Editor: Emmanuel C Besa, MDmore...;)
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Beta Thalassemia
Sections Beta Thalassemia
Overview
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Etiology
Epidemiology
Prognosis
Patient Education
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Presentation
DDx
Workup
Approach Considerations
Laboratory Studies
Prenatal Diagnosis
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DDx
Diagnostic Considerations
A major diagnostic consideration is to distinguish mild microcytic anemia due to beta-thalassemia carrier state from microcytic anemia due to other causes. Iron studies (iron, transferrin, ferritin) are useful in excluding iron deficiency and the anemia of chronic disorders as the cause of the patient's anemia.
Calculation of the Mentzer index (mean corpuscular volume per red cell count) may be helpful. A Mentzer index of less than 13 suggests that the patient has the thalassemia trait, and an index of more than 13 suggests that the patient has iron deficiency.
Alpha thalassemia, which is characterized by genetic defects in the alpha-globin gene, is another known cause of mild microcytic anemia and has features similar to those of beta thalassemia. However, in contrast to beta-thalassemia minor (carrier) patients who have elevated levels of Hb A2 (2 alpha-globin chains complexed with 2 delta-globin chains), patients with alpha-thalassemia have normal levels of Hb.
Establishing the diagnosis of the alpha-thalassemia trait is often a diagnosis of exclusion. Definitive diagnosis requires measuring either the alpha-beta chain synthesis ratio or performing genetic tests of the alpha-globin cluster (using Southern blot or polymerase chain reaction [PCR] assay tests).
Unstable Hb levels and some types of red cell membrane disorders are other conditions to consider in the differential diagnosis of beta-thalassemia.
Differential Diagnoses
Alpha Thalassemia
Anemia of Chronic Disease and Renal Failure
Iron Deficiency Anemia
Lead Nephropathy
Sideroblastic Anemias
Workup
;)
References
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Cappellini MD, Porter J, Origa R, Forni GL, Voskaridou E, Galactéros F, et al. Sotatercept, a novel transforming growth factor β ligand trap, improves anemia in β-thalassemia: a phase II, open-label, dose-finding study. Haematologica. 2019 Mar. 104 (3):477-484. [QxMD MEDLINE Link].[Full Text].
Taher AT, Karakas Z, Cassinerio E, Siritanaratkul N, Kattamis A, Maggio A, et al. Efficacy and safety of ruxolitinib in regularly transfused patients with thalassemia: results from a phase 2a study. Blood. 2018 Jan 11. 131 (2):263-265. [QxMD MEDLINE Link].[Full Text].
Ovsyannikova G, Balashov D, Demina I, Shelikhova L, Pshonkin A, Maschan M, et al. Efficacy and safety of ruxolitinib in ineffective erythropoiesis suppression as a pretransplantation treatment for pediatric patients with beta-thalassemia major. Pediatr Blood Cancer. 2021 Nov. 68 (11):e29338. [QxMD MEDLINE Link].
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Cappellini MD, Porter J, Origa R, Forni GL, Voskaridou E, Galactéros F, et al. Sotatercept, a novel transforming growth factor β ligand trap, improves anemia in β-thalassemia: a phase II, open-label, dose-finding study. Haematologica. 2019 Mar. 104 (3):477-484. [QxMD MEDLINE Link].[Full Text].
Media Gallery
Peripheral smear in beta-zero thalassemia minor showing microcytes (M), target cells (T), and poikilocytes.
Peripheral smear from a patient with beta-zero thalassemia major showing more marked microcytosis (M) and anisopoikilocytosis (P) than in thalassemia minor. Target cells (T) and hypochromia are prominent.
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Author
Pooja Advani, MD Clinical Fellow, Department of Hematology/Oncology, Mayo Clinic
Pooja Advani, MD is a member of the following medical societies: American Society of Hematology, American Society of Clinical Oncology, Florida Society of Clinical Oncology
Disclosure: Nothing to disclose.
Specialty Editor Board
Francisco Talavera, PharmD, PhD Adjunct Assistant Professor, University of Nebraska Medical Center College of Pharmacy; Editor-in-Chief, Medscape Drug Reference
Disclosure: Received salary from Medscape for employment.
Marcel E Conrad, MD Distinguished Professor of Medicine (Retired), University of South Alabama College of Medicine
Marcel E Conrad, MD is a member of the following medical societies: Alpha Omega Alpha, American Association for the Advancement of Science, American Association of Blood Banks, American Chemical Society, American College of Physicians, American Physiological Society, American Society for Clinical Investigation, American Society of Hematology, Association of American Physicians, The Society of Federal Health Professionals (AMSUS), International Society of Hematology, Society for Experimental Biology and Medicine, SWOG
Disclosure: Partner received none from No financial interests for none.
Chief Editor
Emmanuel C Besa, MD Professor Emeritus, Department of Medicine, Division of Hematologic Malignancies and Hematopoietic Stem Cell Transplantation, Kimmel Cancer Center, Jefferson Medical College of Thomas Jefferson University
Emmanuel C Besa, MD is a member of the following medical societies: American Association for Cancer Education, American Society of Clinical Oncology, American College of Clinical Pharmacology, American Federation for Medical Research, American Society of Hematology, New York Academy of Sciences
Disclosure: Nothing to disclose.
Acknowledgements
Kenichi Takeshita, MD Adjunct Associate Professor, Department of Medicine, Division of Hematology, New York University School of Medicine; Medical Director, Clinical Research and Development, Celgene
Kenichi Takeshita, MD is a member of the following medical societies: American Society of Hematology
Disclosure: Nothing to disclose.
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