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proofwiki-10900
Orthogonal Trajectories/Examples/Rectangular Hyperbolas
Consider the one-parameter family of curves of rectangular hyperbolas: :$(1): \quad x y = c$ Its family of orthogonal trajectories is given by the equation: :$x^2 - y^2 = c$ :600px
We use the technique of formation of ordinary differential equation by elimination. Differentiating $(1)$ {{WRT|Differentiation}} $x$ gives: :$x \dfrac {\d y} {\d x} + y = 0$ {{begin-eqn}} {{eqn | l = x \frac {\d y} {\d x} + y | r = 0 | c = }} {{eqn | ll= \leadsto | l = \frac {\d y} {\d x} | r ...
Consider the [[Definition:One-Parameter Family of Curves|one-parameter family of curves]] of [[Definition:Rectangular Hyperbola|rectangular hyperbolas]]: :$(1): \quad x y = c$ Its [[Definition:Orthogonal Trajectories|family of orthogonal trajectories]] is given by the equation: :$x^2 - y^2 = c$ :[[File:RectanguleHy...
We use the technique of [[Definition:Formation of Ordinary Differential Equation by Elimination|formation of ordinary differential equation by elimination]]. [[Definition:Differentiation|Differentiating]] $(1)$ {{WRT|Differentiation}} $x$ gives: :$x \dfrac {\d y} {\d x} + y = 0$ {{begin-eqn}} {{eqn | l = x \frac {\d ...
Orthogonal Trajectories/Examples/Rectangular Hyperbolas
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Rectangular_Hyperbolas
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Rectangular_Hyperbolas
[ "Examples of Orthogonal Trajectories", "Hyperbolas" ]
[ "Definition:Family of Curves/One-Parameter", "Definition:Rectangular Hyperbola", "Definition:Orthogonal Trajectories", "File:RectanguleHyperbolaeOrthogonalTrajectories.png" ]
[ "Definition:Formation of Ordinary Differential Equation by Elimination", "Definition:Differentiation", "Orthogonal Trajectories of One-Parameter Family of Curves", "Definition:Orthogonal Trajectories", "Solution to Separable Differential Equation" ]
proofwiki-10901
Orthogonal Trajectories/Examples/Parabolas Tangent to X Axis
Consider the one-parameter family of curves of parabolas which are tangent to the $x$-axis at the origin: :$(1): \quad y = c x^2$ Its family of orthogonal trajectories is given by the equation: :$x^2 + 2 y^2 = c$ :600px
We use the technique of formation of ordinary differential equation by elimination. Differentiating $(1)$ {{WRT|Differentiation}} $x$ gives: :$x \dfrac {\d y} {\d x} + y = 0$ {{begin-eqn}} {{eqn | n = 2 | l = \frac {\d y} {\d x} | r = 2 c x | c = }} {{eqn | ll= \leadsto | l = \frac {\d y} {\d x...
Consider the [[Definition:One-Parameter Family of Curves|one-parameter family of curves]] of [[Definition:Parabola|parabolas]] which are [[Definition:Tangent Line|tangent]] to the [[Definition:X-Axis|$x$-axis]] at the [[Definition:Origin|origin]]: :$(1): \quad y = c x^2$ Its [[Definition:Orthogonal Trajectories|famil...
We use the technique of [[Definition:Formation of Ordinary Differential Equation by Elimination|formation of ordinary differential equation by elimination]]. [[Definition:Differentiation|Differentiating]] $(1)$ {{WRT|Differentiation}} $x$ gives: :$x \dfrac {\d y} {\d x} + y = 0$ {{begin-eqn}} {{eqn | n = 2 | l ...
Orthogonal Trajectories/Examples/Parabolas Tangent to X Axis
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Parabolas_Tangent_to_X_Axis
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Parabolas_Tangent_to_X_Axis
[ "Examples of Orthogonal Trajectories", "Parabolas" ]
[ "Definition:Family of Curves/One-Parameter", "Definition:Parabola", "Definition:Tangent Line", "Definition:Axis/X-Axis", "Definition:Coordinate System/Origin", "Definition:Orthogonal Trajectories", "File:ParabolasTangentAxisOrthogonalTrajectories.png" ]
[ "Definition:Formation of Ordinary Differential Equation by Elimination", "Definition:Differentiation", "Orthogonal Trajectories of One-Parameter Family of Curves", "Definition:Orthogonal Trajectories", "Solution to Separable Differential Equation" ]
proofwiki-10902
Orthogonal Trajectories/Examples/Cardioids
Consider the one-parameter family of curves of cardioids given in polar form as: :$(1): \quad r = c \paren {1 + \cos \theta}$ Its family of orthogonal trajectories is given by the equation: :$r = c \paren {1 - \cos \theta}$ :600px
We use the technique of formation of ordinary differential equation by elimination. Differentiating $(1)$ {{WRT|Differentiation}} $r$ gives: {{begin-eqn}} {{eqn | n = 2 | l = \frac {\d r} {\d \theta} | r = - c \sin \theta | c = }} {{eqn | ll= \leadsto | l = \frac {\d r} {\d \theta} | r = ...
Consider the [[Definition:One-Parameter Family of Curves|one-parameter family of curves]] of [[Definition:Cardioid|cardioids]] given in [[Definition:Polar Coordinates|polar form]] as: :$(1): \quad r = c \paren {1 + \cos \theta}$ Its [[Definition:Orthogonal Trajectories|family of orthogonal trajectories]] is given by ...
We use the technique of [[Definition:Formation of Ordinary Differential Equation by Elimination|formation of ordinary differential equation by elimination]]. [[Definition:Differentiation|Differentiating]] $(1)$ {{WRT|Differentiation}} $r$ gives: {{begin-eqn}} {{eqn | n = 2 | l = \frac {\d r} {\d \theta} |...
Orthogonal Trajectories/Examples/Cardioids
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Cardioids
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Cardioids
[ "Examples of Orthogonal Trajectories", "Cardioids" ]
[ "Definition:Family of Curves/One-Parameter", "Definition:Cardioid", "Definition:Polar Coordinates", "Definition:Orthogonal Trajectories", "File:CardioidsOrthogonalTrajectories.png" ]
[ "Definition:Formation of Ordinary Differential Equation by Elimination", "Definition:Differentiation", "Orthogonal Trajectories of One-Parameter Family of Curves", "Definition:Orthogonal Trajectories", "Solution to Separable Differential Equation" ]
proofwiki-10903
Orthogonal Trajectories/Examples/Exponential Functions
Consider the one-parameter family of curves of graphs of the exponential function: :$(1): \quad y = c e^x$ Its family of orthogonal trajectories is given by the equation: :$y^2 = -2 x + c$ :600px
We use the technique of formation of ordinary differential equation by elimination. Differentiating $(1)$ {{WRT|Differentiation}} $x$ gives: :$\dfrac {\d y} {\d x} = c e^x$ {{begin-eqn}} {{eqn | n = 2 | l = \frac {\d y} {\d x} | r = c e^x | c = }} {{eqn | ll= \leadsto | l = \frac {\d y} {\d x} ...
Consider the [[Definition:One-Parameter Family of Curves|one-parameter family of curves]] of [[Definition:Graph of Mapping|graphs]] of the [[Definition:Real Exponential Function|exponential function]]: :$(1): \quad y = c e^x$ Its [[Definition:Orthogonal Trajectories|family of orthogonal trajectories]] is given by the...
We use the technique of [[Definition:Formation of Ordinary Differential Equation by Elimination|formation of ordinary differential equation by elimination]]. [[Definition:Differentiation|Differentiating]] $(1)$ {{WRT|Differentiation}} $x$ gives: :$\dfrac {\d y} {\d x} = c e^x$ {{begin-eqn}} {{eqn | n = 2 | l = ...
Orthogonal Trajectories/Examples/Exponential Functions
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Exponential_Functions
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Exponential_Functions
[ "Examples of Orthogonal Trajectories" ]
[ "Definition:Family of Curves/One-Parameter", "Definition:Graph of Mapping", "Definition:Exponential Function/Real", "Definition:Orthogonal Trajectories", "File:ExponentialsOrthogonalTrajectories.png" ]
[ "Definition:Formation of Ordinary Differential Equation by Elimination", "Definition:Differentiation", "Orthogonal Trajectories of One-Parameter Family of Curves", "Definition:Orthogonal Trajectories", "Solution to Separable Differential Equation" ]
proofwiki-10904
Orthogonal Trajectories/Examples/Parabolas with Focus at Origin
Consider the one-parameter family of curves of parabolas whose focus is at the origin and whose axis is the $x$-axis: :$(1): \quad y^2 = 4 c \paren {x + c}$ Its family of orthogonal trajectories is given by the equation: :$y^2 = 4 c \paren {x + c}$ :600px
We use the technique of formation of ordinary differential equation by elimination. Differentiating $(1)$ {{WRT|Differentiation}} $x$ gives: {{begin-eqn}} {{eqn | n = 2 | l = 2 y \frac {\d y} {\d x} | r = 4 c | c = }} {{eqn | ll= \leadsto | l = c | r = \frac y 2 \frac {\d y} {\d x} ...
Consider the [[Definition:One-Parameter Family of Curves|one-parameter family of curves]] of [[Definition:Parabola|parabolas]] whose [[Definition:Focus of Parabola|focus]] is at the [[Definition:Origin|origin]] and whose [[Definition:Axis of Parabola|axis]] is the [[Definition:X-Axis|$x$-axis]]: :$(1): \quad y^2 = 4 c ...
We use the technique of [[Definition:Formation of Ordinary Differential Equation by Elimination|formation of ordinary differential equation by elimination]]. [[Definition:Differentiation|Differentiating]] $(1)$ {{WRT|Differentiation}} $x$ gives: {{begin-eqn}} {{eqn | n = 2 | l = 2 y \frac {\d y} {\d x} | ...
Orthogonal Trajectories/Examples/Parabolas with Focus at Origin
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Parabolas_with_Focus_at_Origin
https://proofwiki.org/wiki/Orthogonal_Trajectories/Examples/Parabolas_with_Focus_at_Origin
[ "Examples of Orthogonal Trajectories" ]
[ "Definition:Family of Curves/One-Parameter", "Definition:Parabola", "Definition:Parabola/Focus", "Definition:Coordinate System/Origin", "Definition:Parabola/Axis", "Definition:Axis/X-Axis", "Definition:Orthogonal Trajectories", "File:ParabolasFocusOriginOrthogonalTrajectories.png" ]
[ "Definition:Formation of Ordinary Differential Equation by Elimination", "Definition:Differentiation", "Orthogonal Trajectories of One-Parameter Family of Curves", "Definition:Orthogonal Trajectories" ]
proofwiki-10905
Half-Life of Radioactive Substance
Let a radioactive element $S$ decay with a rate constant $k$. Then its half-life $T$ is given by: :$T = \dfrac {\ln 2} k$ :400px
Let $x_0$ be the quantity of $S$ at time $t = 0$. At time $t = T$ the quantity of $S$ has been reduced to $x = \dfrac {x_0} 2$. This gives: {{begin-eqn}} {{eqn | l = x_0 e^{-k T} | r = \frac {x_0} 2 | c = First-Order Reaction }} {{eqn | ll= \leadsto | l = e^{k T} | r = 2 | c = }} {{eqn | l...
Let a [[Definition:Radioactive Element|radioactive element]] $S$ [[Definition:Radioactive Decay|decay]] with a [[Definition:Rate Constant|rate constant]] $k$. Then its [[Definition:Half-Life|half-life]] $T$ is given by: :$T = \dfrac {\ln 2} k$ :[[File:HalfLife.png|400px]]
Let $x_0$ be the quantity of $S$ at [[Definition:Time|time]] $t = 0$. At [[Definition:Time|time]] $t = T$ the quantity of $S$ has been reduced to $x = \dfrac {x_0} 2$. This gives: {{begin-eqn}} {{eqn | l = x_0 e^{-k T} | r = \frac {x_0} 2 | c = [[First-Order Reaction]] }} {{eqn | ll= \leadsto | l =...
Half-Life of Radioactive Substance
https://proofwiki.org/wiki/Half-Life_of_Radioactive_Substance
https://proofwiki.org/wiki/Half-Life_of_Radioactive_Substance
[ "Half-Life", "Radioactive Decay" ]
[ "Definition:Radioactive Decay/Radioactive Element", "Definition:Radioactive Decay", "Definition:First-Order Reaction/Rate Constant", "Definition:Radioactive Decay/Half-Life", "File:HalfLife.png" ]
[ "Definition:Time", "Definition:Time", "First-Order Reaction" ]
proofwiki-10906
Density not greater than Weight
Let $T = \struct {S, \tau}$ be a topological space. Then :$\map d T \le \map w T$ where :$\map d T$ denotes the density of $T$, :$\map w T$ denotes the weight of $T$.
By definition of weight there exists a basis $\BB$ of $T$: :$\map w T = \card \BB$ where $\card \BB$ denotes the cardinality of $\BB$. By Axiom of Choice define a mapping $f: \paren {\BB \setminus \O} \to S$: :$\forall U \in \BB: U \ne \O \implies f \sqbrk U \in U$ We will prove that :$\forall U \in \tau: U \ne \O \imp...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Then :$\map d T \le \map w T$ where :$\map d T$ denotes the [[Definition:Density of Topological Space|density]] of $T$, :$\map w T$ denotes the [[Definition:Weight of Topological Space|weight]] of $T$.
By definition of [[Definition:Weight of Topological Space|weight]] there exists a [[Definition:Analytic Basis|basis]] $\BB$ of $T$: :$\map w T = \card \BB$ where $\card \BB$ denotes the [[Definition:Cardinality|cardinality]] of $\BB$. By [[Axiom:Axiom of Choice|Axiom of Choice]] define a [[Definition:Mapping|mapping]]...
Density not greater than Weight
https://proofwiki.org/wiki/Density_not_greater_than_Weight
https://proofwiki.org/wiki/Density_not_greater_than_Weight
[ "Denseness" ]
[ "Definition:Topological Space", "Definition:Density of Topological Space", "Definition:Weight of Topological Space" ]
[ "Definition:Weight of Topological Space", "Definition:Basis (Topology)/Analytic Basis", "Definition:Cardinality", "Axiom:Axiom of Choice", "Definition:Mapping", "Definition:Image (Set Theory)/Mapping/Mapping", "Definition:Empty Set", "Definition:Basis (Topology)/Analytic Basis", "Definition:Image (S...
proofwiki-10907
Temperature of Body under Newton's Law of Cooling
Let $B$ be a body in an environment whose ambient temperature is $H_a$. Let $H$ be the temperature of $B$ at time $t$. Let $H_0$ be the temperature of $B$ at time $t = 0$. Then: :$H = H_a - \paren {H_0 - H_a} e^{-k t}$ where $k$ is some positive constant.
By Newton's Law of Cooling: :The rate at which a hot body loses heat is proportional to the difference in temperature between it and its surroundings. We have the differential equation: :$\dfrac {\d H} {\d t} \propto - \paren {H - H_a}$ That is: :$\dfrac {\d H} {\d t} = - k \paren {H - H_a}$ where $k$ is some positive ...
Let $B$ be a [[Definition:Body|body]] in an environment whose ambient [[Definition:Temperature|temperature]] is $H_a$. Let $H$ be the [[Definition:Temperature|temperature]] of $B$ at time $t$. Let $H_0$ be the [[Definition:Temperature|temperature]] of $B$ at time $t = 0$. Then: :$H = H_a - \paren {H_0 - H_a} e^{-k ...
By [[Newton's Law of Cooling]]: :The [[Definition:Rate|rate]] at which a hot [[Definition:Body|body]] loses [[Definition:Heat|heat]] is [[Definition:Proportion|proportional]] to the difference in [[Definition:Temperature|temperature]] between it and its surroundings. We have the [[Definition:First Order Ordinary Diff...
Temperature of Body under Newton's Law of Cooling
https://proofwiki.org/wiki/Temperature_of_Body_under_Newton's_Law_of_Cooling
https://proofwiki.org/wiki/Temperature_of_Body_under_Newton's_Law_of_Cooling
[ "Thermodynamics" ]
[ "Definition:Body", "Definition:Temperature", "Definition:Temperature", "Definition:Temperature", "Definition:Positive/Real Number", "Definition:Constant" ]
[ "Newton's Law of Cooling", "Definition:Rate", "Definition:Body", "Definition:Heat", "Definition:Proportion", "Definition:Temperature", "Definition:First Order Ordinary Differential Equation", "Definition:Positive/Real Number", "Definition:Constant", "Decay Equation" ]
proofwiki-10908
Speed of Body under Free Fall from Height
Let an object $B$ be released above ground from a point near the Earth's surface and allowed to fall freely. Let $B$ fall a distance $s$. Then: :$v = \sqrt {2 g s}$ where: :$v$ is the speed of $B$ after having fallen a distance $s$ :$g$ is the Acceleration Due to Gravity at the height through which $B$ falls. It is sup...
From Equations of Motion with Constant Acceleration: Velocity after Distance: :$\mathbf v \cdot \mathbf v = \mathbf u \cdot \mathbf u + 2 \mathbf g \cdot \mathbf s$ All dot products are between pairs of parallel vectors. Thus by Cosine Formula for Dot Product: :$v^2 = u^2 + 2 g s$ Here the body falls from rest, so: :$\...
Let an [[Definition:Object|object]] $B$ be released above ground from a point near the [[Definition:Earth|Earth's]] surface and allowed to fall freely. Let $B$ fall a [[Definition:Displacement|distance]] $s$. Then: :$v = \sqrt {2 g s}$ where: :$v$ is the [[Definition:Speed|speed]] of $B$ after having fallen a [[Defin...
From [[Equations of Motion with Constant Acceleration/Velocity after Distance|Equations of Motion with Constant Acceleration: Velocity after Distance]]: :$\mathbf v \cdot \mathbf v = \mathbf u \cdot \mathbf u + 2 \mathbf g \cdot \mathbf s$ All [[Definition:Dot Product|dot products]] are between pairs of [[Definition:...
Speed of Body under Free Fall from Height/Proof 1
https://proofwiki.org/wiki/Speed_of_Body_under_Free_Fall_from_Height
https://proofwiki.org/wiki/Speed_of_Body_under_Free_Fall_from_Height/Proof_1
[ "Mechanics", "Gravity", "Speed of Body under Free Fall from Height" ]
[ "Definition:Object", "Definition:Earth", "Definition:Displacement", "Definition:Speed", "Definition:Displacement", "Acceleration Due to Gravity", "Definition:Constant" ]
[ "Equations of Motion with Constant Acceleration/Velocity after Distance", "Definition:Dot Product", "Definition:Parallel (Geometry)/Lines", "Definition:Vector", "Cosine Formula for Dot Product", "Definition:Stationary" ]
proofwiki-10909
Speed of Body under Free Fall from Height
Let an object $B$ be released above ground from a point near the Earth's surface and allowed to fall freely. Let $B$ fall a distance $s$. Then: :$v = \sqrt {2 g s}$ where: :$v$ is the speed of $B$ after having fallen a distance $s$ :$g$ is the Acceleration Due to Gravity at the height through which $B$ falls. It is sup...
From Acceleration is Second Derivative of Displacement with respect to Time: :$\mathbf g = \dfrac {\d^2 \mathbf s} {\d t^2}$ Integrating with respect to $t$, and by definition of velocity: :$\mathbf v = \dfrac {\d \mathbf s} {\d t} = \mathbf g t + \mathbf c_1$ When $t = 0$, we have that $\mathrm c_1$ is the initial vel...
Let an [[Definition:Object|object]] $B$ be released above ground from a point near the [[Definition:Earth|Earth's]] surface and allowed to fall freely. Let $B$ fall a [[Definition:Displacement|distance]] $s$. Then: :$v = \sqrt {2 g s}$ where: :$v$ is the [[Definition:Speed|speed]] of $B$ after having fallen a [[Defin...
From [[Acceleration is Second Derivative of Displacement with respect to Time]]: :$\mathbf g = \dfrac {\d^2 \mathbf s} {\d t^2}$ [[Definition:Integration|Integrating]] with respect to $t$, and by definition of [[Definition:Velocity|velocity]]: :$\mathbf v = \dfrac {\d \mathbf s} {\d t} = \mathbf g t + \mathbf c_1$ W...
Speed of Body under Free Fall from Height/Proof 2
https://proofwiki.org/wiki/Speed_of_Body_under_Free_Fall_from_Height
https://proofwiki.org/wiki/Speed_of_Body_under_Free_Fall_from_Height/Proof_2
[ "Mechanics", "Gravity", "Speed of Body under Free Fall from Height" ]
[ "Definition:Object", "Definition:Earth", "Definition:Displacement", "Definition:Speed", "Definition:Displacement", "Acceleration Due to Gravity", "Definition:Constant" ]
[ "Acceleration is Second Derivative of Displacement with respect to Time", "Definition:Primitive (Calculus)/Integration", "Definition:Velocity", "Definition:Velocity", "Definition:Primitive (Calculus)/Integration", "Definition:Displacement", "Definition:Stationary" ]
proofwiki-10910
Speed of Body under Free Fall from Height
Let an object $B$ be released above ground from a point near the Earth's surface and allowed to fall freely. Let $B$ fall a distance $s$. Then: :$v = \sqrt {2 g s}$ where: :$v$ is the speed of $B$ after having fallen a distance $s$ :$g$ is the Acceleration Due to Gravity at the height through which $B$ falls. It is sup...
From the Principle of Conservation of Energy: :$K + P = C$ where: :$K$ is the kinetic energy of $B$ :$P$ is the potential energy of $B$ :$C$ is a constant. Let the mass of $B$ be $m$. From Kinetic Energy of Motion: :$K = \dfrac {m v^2} 2$ where $v$ is the speed of $B$. From Potential Energy of Position: :$P = m g s$ wh...
Let an [[Definition:Object|object]] $B$ be released above ground from a point near the [[Definition:Earth|Earth's]] surface and allowed to fall freely. Let $B$ fall a [[Definition:Displacement|distance]] $s$. Then: :$v = \sqrt {2 g s}$ where: :$v$ is the [[Definition:Speed|speed]] of $B$ after having fallen a [[Defin...
From the [[Principle of Conservation of Energy]]: :$K + P = C$ where: :$K$ is the [[Definition:Kinetic Energy|kinetic energy]] of $B$ :$P$ is the [[Definition:Potential Energy|potential energy]] of $B$ :$C$ is a [[Definition:Constant|constant]]. Let the [[Definition:Mass|mass]] of $B$ be $m$. From [[Kinetic Energy of...
Speed of Body under Free Fall from Height/Proof 3
https://proofwiki.org/wiki/Speed_of_Body_under_Free_Fall_from_Height
https://proofwiki.org/wiki/Speed_of_Body_under_Free_Fall_from_Height/Proof_3
[ "Mechanics", "Gravity", "Speed of Body under Free Fall from Height" ]
[ "Definition:Object", "Definition:Earth", "Definition:Displacement", "Definition:Speed", "Definition:Displacement", "Acceleration Due to Gravity", "Definition:Constant" ]
[ "Principle of Conservation of Energy", "Definition:Kinetic Energy", "Definition:Potential Energy", "Definition:Constant", "Definition:Mass", "Kinetic Energy of Motion", "Definition:Speed", "Potential Energy of Position", "Definition:Distance", "Definition:Stationary", "Definition:Kinetic Energy"...
proofwiki-10911
Terminal Speed of Body under Fall Retarded Proportional to Speed
Let $B$ be a body falling in a gravitational field. Let $B$ be falling through a medium which exerts a resisting force $k \mathbf v$ upon $B$ which is proportional to the speed of $B$ relative to the medium. Then the terminal speed of $B$ is given by: :$v = \dfrac {g m} k$
Let $B$ start from rest. From Motion of Body Falling through Air, the differential equation governing the motion of $B$ is given by: :$m \dfrac {\d^2 \mathbf s} {\d t^2} = m \mathbf g - k \dfrac {\d \mathbf s} {\d t}$ Dividing through by $m$ and setting $c = \dfrac k m$ gives: :$\dfrac {\d^2 \mathbf s} {\d t^2} = \math...
Let $B$ be a [[Definition:Body|body]] falling in a [[Definition:Gravitational Field|gravitational field]]. Let $B$ be falling through a medium which exerts a resisting [[Definition:Force|force]] $k \mathbf v$ upon $B$ which is [[Definition:Proportion|proportional]] to the [[Definition:Speed|speed]] of $B$ relative to ...
Let $B$ start from [[Definition:Stationary|rest]]. From [[Motion of Body Falling through Air]], the [[Definition:Differential Equation|differential equation]] governing the motion of $B$ is given by: :$m \dfrac {\d^2 \mathbf s} {\d t^2} = m \mathbf g - k \dfrac {\d \mathbf s} {\d t}$ Dividing through by $m$ and sett...
Terminal Speed of Body under Fall Retarded Proportional to Speed
https://proofwiki.org/wiki/Terminal_Speed_of_Body_under_Fall_Retarded_Proportional_to_Speed
https://proofwiki.org/wiki/Terminal_Speed_of_Body_under_Fall_Retarded_Proportional_to_Speed
[ "Terminal Speed", "Mechanics" ]
[ "Definition:Body", "Definition:Gravitational Field", "Definition:Force", "Definition:Proportion", "Definition:Speed", "Definition:Terminal Speed" ]
[ "Definition:Stationary", "Motion of Body Falling through Air", "Definition:Differential Equation", "Definition:Velocity", "Definition:Magnitude" ]
proofwiki-10912
Approximate Motion of Simple Pendulum
Consider a simple pendulum consisting of a bob whose mass is $m$, at the end of a rod of negligible mass of length $a$. Let the bob be pulled to one side so that the rod is at a small angle $\alpha$ (less than about $10 \degrees$ or $15 \degrees$) from the vertical and then released. Let $T$ be the period of the pendul...
At a time $t$, let: :the rod be at an angle $\theta$ to the the vertical :the bob be travelling at a speed $v$ :the displacement of the bob from where it is when the rod is vertical, along its line of travel, be $s$. :350px From Motion of Simple Pendulum, the equation of motion of the bob is given by: :$\dfrac {a^2} 2 ...
Consider a [[Definition:Simple Pendulum|simple pendulum]] consisting of a [[Definition:Pendulum Bob|bob]] whose [[Definition:Mass|mass]] is $m$, at the end of a [[Definition:Rod|rod]] of negligible [[Definition:Mass|mass]] of [[Definition:Length (Linear Measure)|length]] $a$. Let the [[Definition:Pendulum Bob|bob]] be...
At a time $t$, let: :the [[Definition:Rod|rod]] be at an [[Definition:Angle|angle]] $\theta$ to the [[Definition:Vertical|the vertical]] :the [[Definition:Pendulum Bob|bob]] be travelling at a [[Definition:Speed|speed]] $v$ :the [[Definition:Displacement|displacement]] of the [[Definition:Pendulum Bob|bob]] from where ...
Approximate Motion of Simple Pendulum
https://proofwiki.org/wiki/Approximate_Motion_of_Simple_Pendulum
https://proofwiki.org/wiki/Approximate_Motion_of_Simple_Pendulum
[ "Simple Pendulums", "Mechanics" ]
[ "Definition:Pendulum/Simple", "Definition:Simple Pendulum/Bob", "Definition:Mass", "Definition:Rod", "Definition:Mass", "Definition:Linear Measure/Length", "Definition:Simple Pendulum/Bob", "Definition:Rod", "Definition:Angle", "Definition:Vertical", "Definition:Simple Pendulum/Period", "Defin...
[ "Definition:Rod", "Definition:Angle", "Definition:Vertical", "Definition:Simple Pendulum/Bob", "Definition:Speed", "Definition:Displacement", "Definition:Simple Pendulum/Bob", "Definition:Rod", "Definition:Vertical Line", "File:MotionOfPendulum.png", "Motion of Simple Pendulum", "Definition:Si...
proofwiki-10913
Space is Separable iff Density not greater than Aleph Zero
Let $T$ be a topological space. Then: :$T$ is separable {{iff}} $\map d T \le \aleph_0$ where :$\map d T$ denotes the density of $T$, :$\aleph$ denotes the aleph mapping.
:$T$ is separable {{iff}}: :there exists a countable subset of $T$ which is dense by definition of separable space {{iff}}: :there exists a subset $A$ of $T$ such that $A$ is dense and exists an injection $A \to \N$ by definition of countable set {{iff}}: :there exists a subset $A$ of $T$ such that $A$ is dense and $\c...
Let $T$ be a [[Definition:Topological Space|topological space]]. Then: :$T$ is [[Definition:Separable Space|separable]] {{iff}} $\map d T \le \aleph_0$ where :$\map d T$ denotes the [[Definition:Density of Topological Space|density]] of $T$, :$\aleph$ denotes the [[Definition:Aleph Mapping|aleph mapping]].
:$T$ is [[Definition:Separable Space|separable]] {{iff}}: :there exists a [[Definition:Countable Set|countable]] [[Definition:Subset|subset]] of $T$ which is [[Definition:Everywhere Dense|dense]] by definition of [[Definition:Separable Space|separable space]] {{iff}}: :there exists a [[Definition:Subset|subset]] $A$ of...
Space is Separable iff Density not greater than Aleph Zero
https://proofwiki.org/wiki/Space_is_Separable_iff_Density_not_greater_than_Aleph_Zero
https://proofwiki.org/wiki/Space_is_Separable_iff_Density_not_greater_than_Aleph_Zero
[ "Denseness", "Separable Spaces" ]
[ "Definition:Topological Space", "Definition:Separable Space", "Definition:Density of Topological Space", "Definition:Aleph Mapping" ]
[ "Definition:Separable Space", "Definition:Countable Set", "Definition:Subset", "Definition:Everywhere Dense", "Definition:Separable Space", "Definition:Subset", "Definition:Everywhere Dense", "Definition:Injection", "Definition:Countable Set", "Definition:Subset", "Definition:Everywhere Dense", ...
proofwiki-10914
Boundary of Union of Separated Sets equals Union of Boundaries
Let $T$ be a topological space. Let $A, B$ be subsets of $T$. Let $A$ and $B$ are separated. Then: :$\map \partial {A \cup B} = \partial A \cup \partial B$ where: :$\partial A$ denotes the boundary of $A$ :$A \cup B$ denotes the union of $A$ and $B$.
By definition of separated sets: :$(1): \quad A^- \cap B = A \cap B^- = \O$ By Separated Sets are Disjoint: :$A \cap B = \O$ {{begin-eqn}} {{eqn | l = \partial A \cup \partial B | r = \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B} | c = Union of Boundaries }}...
Let $T$ be a [[Definition:Topological Space|topological space]]. Let $A, B$ be [[Definition:Subset|subsets]] of $T$. Let $A$ and $B$ are [[Definition:Separated Sets|separated]]. Then: :$\map \partial {A \cup B} = \partial A \cup \partial B$ where: :$\partial A$ denotes the [[Definition:Boundary (Topology)|boundary]]...
By definition of [[Definition:Separated Sets|separated sets]]: :$(1): \quad A^- \cap B = A \cap B^- = \O$ By [[Separated Sets are Disjoint]]: :$A \cap B = \O$ {{begin-eqn}} {{eqn | l = \partial A \cup \partial B | r = \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B...
Boundary of Union of Separated Sets equals Union of Boundaries
https://proofwiki.org/wiki/Boundary_of_Union_of_Separated_Sets_equals_Union_of_Boundaries
https://proofwiki.org/wiki/Boundary_of_Union_of_Separated_Sets_equals_Union_of_Boundaries
[ "Separated Sets", "Set Boundaries" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Separated Sets", "Definition:Boundary (Topology)", "Definition:Set Union" ]
[ "Definition:Separated Sets", "Separated Sets are Disjoint", "Union of Boundaries", "Boundary of Empty Set is Empty", "Union with Empty Set", "Definition:Set Intersection", "Boundary is Intersection of Closure with Closure of Complement", "Definition:Closure (Topology)", "Definition:Relative Compleme...
proofwiki-10915
Boundary of Empty Set is Empty
Let $T$ be a topological space. Then: :$\partial_T \O = \O$ where $\partial_T \O$ denotes the boundary in topology $T$ of $\O$.
By Boundary is Intersection of Closure with Closure of Complement: :$\partial_T \O = \O^- \cap \relcomp T \O^-$ where $\O^-$ denotes the closure of $\O$. By Closure of Empty Set is Empty Set: :$\O^- = \O$ Thus the result follows by Intersection with Empty Set. {{qed}}
Let $T$ be a [[Definition:Topological Space|topological space]]. Then: :$\partial_T \O = \O$ where $\partial_T \O$ denotes the [[Definition:Boundary (Topology)|boundary]] in topology $T$ of $\O$.
By [[Boundary is Intersection of Closure with Closure of Complement]]: :$\partial_T \O = \O^- \cap \relcomp T \O^-$ where $\O^-$ denotes the [[Definition:Closure (Topology)|closure]] of $\O$. By [[Closure of Empty Set is Empty Set]]: :$\O^- = \O$ Thus the result follows by [[Intersection with Empty Set]]. {{qed}}
Boundary of Empty Set is Empty/Proof 1
https://proofwiki.org/wiki/Boundary_of_Empty_Set_is_Empty
https://proofwiki.org/wiki/Boundary_of_Empty_Set_is_Empty/Proof_1
[ "Set Boundaries", "Boundary of Empty Set is Empty" ]
[ "Definition:Topological Space", "Definition:Boundary (Topology)" ]
[ "Boundary is Intersection of Closure with Closure of Complement", "Definition:Closure (Topology)", "Closure of Empty Set is Empty Set", "Intersection with Empty Set" ]
proofwiki-10916
Boundary of Empty Set is Empty
Let $T$ be a topological space. Then: :$\partial_T \O = \O$ where $\partial_T \O$ denotes the boundary in topology $T$ of $\O$.
From Open and Closed Sets in Topological Space, $\O$ is clopen in $T$. The result follows from Set is Clopen iff Boundary is Empty. {{qed}}
Let $T$ be a [[Definition:Topological Space|topological space]]. Then: :$\partial_T \O = \O$ where $\partial_T \O$ denotes the [[Definition:Boundary (Topology)|boundary]] in topology $T$ of $\O$.
From [[Open and Closed Sets in Topological Space]], $\O$ is [[Definition:Clopen Set|clopen]] in $T$. The result follows from [[Set is Clopen iff Boundary is Empty]]. {{qed}}
Boundary of Empty Set is Empty/Proof 2
https://proofwiki.org/wiki/Boundary_of_Empty_Set_is_Empty
https://proofwiki.org/wiki/Boundary_of_Empty_Set_is_Empty/Proof_2
[ "Set Boundaries", "Boundary of Empty Set is Empty" ]
[ "Definition:Topological Space", "Definition:Boundary (Topology)" ]
[ "Open and Closed Sets in Topological Space", "Definition:Clopen Set", "Set is Clopen iff Boundary is Empty" ]
proofwiki-10917
Terminal Speed of Body under Fall Retarded Proportional to Square of Speed
Let $B$ be a body falling in a gravitational field. Let $B$ be falling through a medium which exerts a resisting force of magnitude $k v^2$ upon $B$ which is proportional to the square of the speed of $B$ relative to the medium. Then the terminal speed of $B$ is given by: :$v = \sqrt {\dfrac {g m} k}$
Let $B$ start from rest. The differential equation governing the motion of $B$ is given by: :$m \dfrac {\d^2 \mathbf s} {\d t^2} = m \mathbf g - k \paren {\dfrac {\d \mathbf s} {\d t} }^2$ Dividing through by $m$ and setting $c = \dfrac k m$ gives: :$\dfrac {\d^2 \mathbf s} {\d t^2} = \mathbf g - c \paren {\dfrac {\d \...
Let $B$ be a [[Definition:Body|body]] falling in a [[Definition:Gravitational Field|gravitational field]]. Let $B$ be falling through a medium which exerts a resisting [[Definition:Force|force]] of [[Definition:Magnitude|magnitude]] $k v^2$ upon $B$ which is [[Definition:Proportion|proportional]] to the [[Definition:S...
Let $B$ start from [[Definition:Stationary|rest]]. The [[Definition:Differential Equation|differential equation]] governing the motion of $B$ is given by: :$m \dfrac {\d^2 \mathbf s} {\d t^2} = m \mathbf g - k \paren {\dfrac {\d \mathbf s} {\d t} }^2$ Dividing through by $m$ and setting $c = \dfrac k m$ gives: :$\d...
Terminal Speed of Body under Fall Retarded Proportional to Square of Speed
https://proofwiki.org/wiki/Terminal_Speed_of_Body_under_Fall_Retarded_Proportional_to_Square_of_Speed
https://proofwiki.org/wiki/Terminal_Speed_of_Body_under_Fall_Retarded_Proportional_to_Square_of_Speed
[ "Terminal Speed", "Mechanics" ]
[ "Definition:Body", "Definition:Gravitational Field", "Definition:Force", "Definition:Magnitude", "Definition:Proportion", "Definition:Square/Function", "Definition:Speed", "Definition:Terminal Speed" ]
[ "Definition:Stationary", "Definition:Differential Equation", "Definition:Velocity", "Definition:Constant", "Definition:Magnitude", "Primitive of Reciprocal of a squared minus x squared/Logarithm Form" ]
proofwiki-10918
Escape Speed of Projectile Fired Upwards
Let $P$ be a planet. Let $P$ have an acceleration due to gravity at its surface of $g$. Let $P$ have a radius of $R$. Then the escape speed of $P$ is given by: :$V = \sqrt {2 g R}$
Let a projectile $B$ of mass $m$ be fired vertically upwards from the surface of $P$ at such a speed that it escapes the gravitational field of $P$ completely. $F$ be the force exerted on $B$ by the gravitational field of $P$. Let $x$ be the distance of $B$ from the surface of $P$ at time $t$. We have: :$F = -\dfrac k ...
Let $P$ be a [[Definition:Planet|planet]]. Let $P$ have an [[Acceleration Due to Gravity|acceleration due to gravity]] at its [[Definition:Surface|surface]] of $g$. Let $P$ have a [[Definition:Radius of Sphere|radius]] of $R$. Then the [[Definition:Escape Speed|escape speed]] of $P$ is given by: :$V = \sqrt {2 g R}...
Let a [[Definition:Projectile|projectile]] $B$ of [[Definition:Mass|mass]] $m$ be fired [[Definition:Vertical Line|vertically]] upwards from the [[Definition:Surface|surface]] of $P$ at such a [[Definition:Speed|speed]] that it escapes the [[Definition:Gravitational Field|gravitational field]] of $P$ completely. $F$ b...
Escape Speed of Projectile Fired Upwards/Proof 1
https://proofwiki.org/wiki/Escape_Speed_of_Projectile_Fired_Upwards
https://proofwiki.org/wiki/Escape_Speed_of_Projectile_Fired_Upwards/Proof_1
[ "Escape Speed of Projectile Fired Upwards", "Escape Speed", "Projectiles", "Ballistics" ]
[ "Definition:Planet", "Acceleration Due to Gravity", "Definition:Surface", "Definition:Sphere/Geometry/Radius", "Definition:Escape Speed" ]
[ "Definition:Projectile", "Definition:Mass", "Definition:Vertical Line", "Definition:Surface", "Definition:Speed", "Definition:Gravitational Field", "Definition:Force", "Definition:Gravitational Field", "Definition:Time", "Definition:Speed", "Definition:Time", "Definition:Speed" ]
proofwiki-10919
Union of Boundaries
Let $T = \struct {S, \tau}$ be a topological space. Let $A, B$ be subsets of $S$. Then: :$\partial A \cup \partial B = \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B}$ where $\partial A$ denotes the boundary of $A$.
First we will prove that :$\partial A \subseteq \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B}$ Let $x \in \partial A$. {{AimForCont}} that :$x \notin \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B}$ Then by definition of u...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Let $A, B$ be [[Definition:Subset|subsets]] of $S$. Then: :$\partial A \cup \partial B = \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B}$ where $\partial A$ denotes the [[Definition:Bou...
First we will prove that :$\partial A \subseteq \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B}$ Let $x \in \partial A$. {{AimForCont}} that :$x \notin \map \partial {A \cup B} \cup \map \partial {A \cap B} \cup \paren {\partial A \cap \partial B}$ Then by definition o...
Union of Boundaries
https://proofwiki.org/wiki/Union_of_Boundaries
https://proofwiki.org/wiki/Union_of_Boundaries
[ "Set Boundaries" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Boundary (Topology)" ]
[ "Definition:Set Union", "Characterization of Boundary by Open Sets", "Intersection Distributes over Union", "De Morgan's Laws (Set Theory)/Relative Complement/Complement of Union", "Definition:Set Intersection", "Characterization of Boundary by Open Sets", "Characterization of Boundary by Open Sets", ...
proofwiki-10920
Length of Arch of Sine Function
The length of one arch of the sine function: :$y = \sin x$ is given by: :$L = 2 \sqrt 2 \map E {\dfrac {\sqrt 2} 2}$ where $E$ denotes the incomplete elliptic integral of the second kind.
Let $L$ be the length of one arch of $y = \sin x$. Then: {{begin-eqn}} {{eqn | l = L | r = 2 \int_0^{\pi/2} \sqrt {1 + \paren {\map {\frac \d {\d x} } {\sin x} }^2} \rd x | c = {{Defof|Length of Curve}} }} {{eqn | r = 2 \int_0^{\pi/2} \sqrt {1 + \cos^2 x} \rd x | c = Derivative of Sine Function }} {{e...
The [[Definition:Length of Curve|length]] of one [[Definition:Arch of Sine Function|arch]] of the [[Definition:Sine Function|sine function]]: :$y = \sin x$ is given by: :$L = 2 \sqrt 2 \map E {\dfrac {\sqrt 2} 2}$ where $E$ denotes the [[Definition:Complete Elliptic Integral of the Second Kind|incomplete elliptic int...
Let $L$ be the [[Definition:Length of Curve|length]] of one [[Definition:Arch of Sine Function|arch]] of $y = \sin x$. Then: {{begin-eqn}} {{eqn | l = L | r = 2 \int_0^{\pi/2} \sqrt {1 + \paren {\map {\frac \d {\d x} } {\sin x} }^2} \rd x | c = {{Defof|Length of Curve}} }} {{eqn | r = 2 \int_0^{\pi/2} \sq...
Length of Arch of Sine Function
https://proofwiki.org/wiki/Length_of_Arch_of_Sine_Function
https://proofwiki.org/wiki/Length_of_Arch_of_Sine_Function
[ "Sine Function", "Complete Elliptic Integral of the Second Kind" ]
[ "Definition:Arc Length", "Definition:Sine/Real Function/Arch", "Definition:Sine", "Definition:Elliptic Integral of the Second Kind/Complete" ]
[ "Definition:Arc Length", "Definition:Sine/Real Function/Arch", "Derivative of Sine Function", "Sum of Squares of Sine and Cosine" ]
proofwiki-10921
Length of Lemniscate of Bernoulli
The total length of the lemniscate of Bernoulli given in polar coordinates as: :$r^2 = a^2 \cos 2 \theta$ is given by: {{begin-eqn}} {{eqn | l = L | r = 4 a \map F {\sqrt 2, \dfrac \pi 4} | c = }} {{eqn | r = \dfrac 1 {\sqrt {2 \pi} } \paren {\map \Gamma {\dfrac 1 4} }^2 | c = }} {{end-eqn}} where $...
The arc length of a small length increment $\d s$ is given in polar co-ordinates by: :$\paren {\d s}^2 = \paren {r \rd \theta}^2 + \paren {\d r}^2$ from which: :$\dfrac {\d s} {\d \theta} = \sqrt {r^2 + \paren {\dfrac {\d r} {\d \theta} }^2}$ Half of one lobe of the lemniscate is achieved when $\theta$ goes from $0$ to...
The total [[Definition:Length of Curve|length]] of the [[Definition:Lemniscate of Bernoulli|lemniscate of Bernoulli]] given in [[Definition:Polar Coordinates|polar coordinates]] as: :$r^2 = a^2 \cos 2 \theta$ is given by: {{begin-eqn}} {{eqn | l = L | r = 4 a \map F {\sqrt 2, \dfrac \pi 4} | c = }} {{eqn ...
The [[Definition:Length of Curve|arc length]] of a small length increment $\d s$ is given in [[Definition:Polar Coordinates|polar co-ordinates]] by: :$\paren {\d s}^2 = \paren {r \rd \theta}^2 + \paren {\d r}^2$ from which: :$\dfrac {\d s} {\d \theta} = \sqrt {r^2 + \paren {\dfrac {\d r} {\d \theta} }^2}$ Half of on...
Length of Lemniscate of Bernoulli
https://proofwiki.org/wiki/Length_of_Lemniscate_of_Bernoulli
https://proofwiki.org/wiki/Length_of_Lemniscate_of_Bernoulli
[ "Lemniscate of Bernoulli", "Incomplete Elliptic Integral of the First Kind" ]
[ "Definition:Arc Length", "Definition:Lemniscate of Bernoulli", "Definition:Polar Coordinates", "Definition:Elliptic Integral of the First Kind/Incomplete" ]
[ "Definition:Arc Length", "Definition:Polar Coordinates", "Definition:Lemniscate of Bernoulli/Lobe", "Definition:Lemniscate of Bernoulli", "Definition:Arc Length", "Definition:Lemniscate of Bernoulli", "Sum of Squares of Sine and Cosine" ]
proofwiki-10922
Boundary of Union is Subset of Union of Boundaries
Let $T = \struct {S, \tau}$ be a topological space. Let $A, B$ be subsets of $S$. Then: :$\map \partial {A \cup B} \subseteq \partial A \cup \partial B$ where $\partial A$ denotes the boundary of $A$.
By Intersection is Subset: :$\relcomp S A \cap \relcomp S B \subseteq \relcomp S A \land \relcomp S A \cap \relcomp S B \subseteq \relcomp S B$ Then by Topological Closure of Subset is Subset of Topological Closure: :$\paren {\relcomp S A \cap \relcomp S B}^- \subseteq \paren {\relcomp S A}^- \land \paren {\relcomp S A...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Let $A, B$ be [[Definition:Subset|subsets]] of $S$. Then: :$\map \partial {A \cup B} \subseteq \partial A \cup \partial B$ where $\partial A$ denotes the [[Definition:Boundary (Topology)|boundary]] of $A$.
By [[Intersection is Subset]]: :$\relcomp S A \cap \relcomp S B \subseteq \relcomp S A \land \relcomp S A \cap \relcomp S B \subseteq \relcomp S B$ Then by [[Topological Closure of Subset is Subset of Topological Closure]]: :$\paren {\relcomp S A \cap \relcomp S B}^- \subseteq \paren {\relcomp S A}^- \land \paren {\re...
Boundary of Union is Subset of Union of Boundaries
https://proofwiki.org/wiki/Boundary_of_Union_is_Subset_of_Union_of_Boundaries
https://proofwiki.org/wiki/Boundary_of_Union_is_Subset_of_Union_of_Boundaries
[ "Set Boundaries" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Boundary (Topology)" ]
[ "Intersection is Subset", "Topological Closure of Subset is Subset of Topological Closure", "Boundary is Intersection of Closure with Closure of Complement", "Boundary is Intersection of Closure with Closure of Complement", "De Morgan's Laws (Set Theory)/Relative Complement/Complement of Union", "Closure ...
proofwiki-10923
Boundary of Intersection is Subset of Union of Boundaries
Let $T = \struct {S, \tau}$ be a topological space. Let $A, B$ be subsets of $S$. Then: :$\map \partial {A \cap B} \subseteq \partial A \cup \partial B$ where $\partial A$ denotes the boundary of $A$.
By Intersection is Subset: :$A \cap B \subseteq A \land A \cap B \subseteq B$ Then by Topological Closure of Subset is Subset of Topological Closure: :$\paren {A \cap B}^- \subseteq A^- \land \paren {A \cap B}^- \subseteq B^-$ Hence by Boundary is Intersection of Closure with Closure of Complement: :$\paren {A \cap B}^...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Let $A, B$ be [[Definition:Subset|subsets]] of $S$. Then: :$\map \partial {A \cap B} \subseteq \partial A \cup \partial B$ where $\partial A$ denotes the [[Definition:Boundary (Topology)|boundary]] of $A$.
By [[Intersection is Subset]]: :$A \cap B \subseteq A \land A \cap B \subseteq B$ Then by [[Topological Closure of Subset is Subset of Topological Closure]]: :$\paren {A \cap B}^- \subseteq A^- \land \paren {A \cap B}^- \subseteq B^-$ Hence by [[Boundary is Intersection of Closure with Closure of Complement]]: :$\par...
Boundary of Intersection is Subset of Union of Boundaries
https://proofwiki.org/wiki/Boundary_of_Intersection_is_Subset_of_Union_of_Boundaries
https://proofwiki.org/wiki/Boundary_of_Intersection_is_Subset_of_Union_of_Boundaries
[ "Set Boundaries" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Boundary (Topology)" ]
[ "Intersection is Subset", "Topological Closure of Subset is Subset of Topological Closure", "Boundary is Intersection of Closure with Closure of Complement", "Boundary is Intersection of Closure with Closure of Complement", "De Morgan's Laws (Set Theory)/Relative Complement/Complement of Intersection", "C...
proofwiki-10924
Complete Elliptic Integral of the First Kind as Power Series
The '''complete elliptic integral of the first kind''': :$\ds \map K k = \int_0^{\pi / 2} \frac {\rd \phi} {\sqrt {1 - k^2 \sin^2 \phi} } = \int_0^1 \frac {\rd v} {\sqrt {\paren {1 - v^2} \paren {1 - k^2 v^2} } }$ can be expressed as the power series: {{begin-eqn}} {{eqn | l = \map K k | r = \frac \pi 2 \sum_{i \...
From Reduction Formula for Integral of Power of Sine, $\forall i \in \N$: {{begin-eqn}} {{eqn | l = \int_0^{\pi / 2} \sin^{2 i} \phi \rd \phi | r = \frac {2 i - 1} {2 i} \int_0^{\pi / 2} \sin^{2 i - 2} \phi \rd \phi - \intlimits {\frac {\sin^{2 i - 1} x \cos x} i} {x = 0} {x = \frac \pi 2} }} {{eqn | r = \frac {2...
The '''[[Definition:Complete Elliptic Integral of the First Kind|complete elliptic integral of the first kind]]''': :$\ds \map K k = \int_0^{\pi / 2} \frac {\rd \phi} {\sqrt {1 - k^2 \sin^2 \phi} } = \int_0^1 \frac {\rd v} {\sqrt {\paren {1 - v^2} \paren {1 - k^2 v^2} } }$ can be expressed as the [[Definition:Power Se...
From [[Reduction Formula for Integral of Power of Sine]], $\forall i \in \N$: {{begin-eqn}} {{eqn | l = \int_0^{\pi / 2} \sin^{2 i} \phi \rd \phi | r = \frac {2 i - 1} {2 i} \int_0^{\pi / 2} \sin^{2 i - 2} \phi \rd \phi - \intlimits {\frac {\sin^{2 i - 1} x \cos x} i} {x = 0} {x = \frac \pi 2} }} {{eqn | r = \fr...
Complete Elliptic Integral of the First Kind as Power Series
https://proofwiki.org/wiki/Complete_Elliptic_Integral_of_the_First_Kind_as_Power_Series
https://proofwiki.org/wiki/Complete_Elliptic_Integral_of_the_First_Kind_as_Power_Series
[ "Complete Elliptic Integral of the First Kind" ]
[ "Definition:Elliptic Integral of the First Kind/Complete", "Definition:Power Series" ]
[ "Reduction Formula for Integral of Power of Sine", "Binomial Theorem/General Binomial Theorem" ]
proofwiki-10925
Complete Elliptic Integral of the Second Kind as Power Series
The '''complete elliptic integral of the second kind''': :$\ds \map E k = \int_0^{\pi / 2} \sqrt {1 - k^2 \sin^2 \phi} \, \rd \phi = \int_0^1 \dfrac {\sqrt {1 - k^2 v^2} } {\sqrt {1 - v^2}} \, \rd v$ can be expressed as the power series: {{begin-eqn}} {{eqn | l = \map E k | r = \frac \pi 2 \sum_{i \mathop \ge 0} ...
From Reduction Formula for Integral of Power of Sine, $\forall i \in \N$: {{begin-eqn}} {{eqn | l = \int_0^{\pi / 2} \sin^{2 i} \phi \rd \phi | r = \frac {2 i - 1} {2 i} \int_0^{\pi / 2} \sin^{2 i - 2} \phi \rd \phi - \intlimits {\frac {\sin^{2 i - 1} x \cos x} i} {x = 0} {x = \frac \pi 2} }} {{eqn | r = \frac {2...
The '''[[Definition:Complete Elliptic Integral of the Second Kind|complete elliptic integral of the second kind]]''': :$\ds \map E k = \int_0^{\pi / 2} \sqrt {1 - k^2 \sin^2 \phi} \, \rd \phi = \int_0^1 \dfrac {\sqrt {1 - k^2 v^2} } {\sqrt {1 - v^2}} \, \rd v$ can be expressed as the [[Definition:Power Series|power se...
From [[Reduction Formula for Integral of Power of Sine]], $\forall i \in \N$: {{begin-eqn}} {{eqn | l = \int_0^{\pi / 2} \sin^{2 i} \phi \rd \phi | r = \frac {2 i - 1} {2 i} \int_0^{\pi / 2} \sin^{2 i - 2} \phi \rd \phi - \intlimits {\frac {\sin^{2 i - 1} x \cos x} i} {x = 0} {x = \frac \pi 2} }} {{eqn | r = \fr...
Complete Elliptic Integral of the Second Kind as Power Series
https://proofwiki.org/wiki/Complete_Elliptic_Integral_of_the_Second_Kind_as_Power_Series
https://proofwiki.org/wiki/Complete_Elliptic_Integral_of_the_Second_Kind_as_Power_Series
[ "Complete Elliptic Integral of the Second Kind" ]
[ "Definition:Elliptic Integral of the Second Kind/Complete", "Definition:Power Series" ]
[ "Reduction Formula for Integral of Power of Sine", "Binomial Theorem/General Binomial Theorem" ]
proofwiki-10926
Discrete Space is Separable iff Countable
Let $T = \struct {S, \tau}$ be a discrete topological space. Then: :$T$ is separable {{iff}} $S$ is countable.
=== Sufficient Condition === Immediate from Separable Discrete Space is Countable. {{qed|lemma}}
Let $T = \struct {S, \tau}$ be a [[Definition:Discrete Space|discrete]] [[Definition:Topological Space|topological space]]. Then: :$T$ is [[Definition:Separable Space|separable]] {{iff}} $S$ is [[Definition:Countable Set|countable]].
=== Sufficient Condition === Immediate from [[Separable Discrete Space is Countable]]. {{qed|lemma}}
Discrete Space is Separable iff Countable
https://proofwiki.org/wiki/Discrete_Space_is_Separable_iff_Countable
https://proofwiki.org/wiki/Discrete_Space_is_Separable_iff_Countable
[ "Discrete Topologies", "Examples of Separable Spaces" ]
[ "Definition:Discrete Topology", "Definition:Topological Space", "Definition:Separable Space", "Definition:Countable Set" ]
[ "Separable Discrete Space is Countable" ]
proofwiki-10927
Set is Countable iff Cardinality not greater Aleph Zero
Let $X$ be a set. Then: :$X$ is countable {{iff}} $\size X \le \aleph_0$ where :$\size X$ denotes the cardinality of $X$, :$\aleph$ denotes the aleph mapping.
:$X$ is countable {{iff}} :there exists an injection $X \to \N$ by definition of countable set {{iff}} :$\size X \le \size \N$ by Injection iff Cardinal Inequality {{iff}} :$\size X \le \aleph_0$ by Aleph Zero equals Cardinality of Naturals. {{qed}} Category:Countable Sets odwikgixvfndjekh3c1vm2d04dez9q6
Let $X$ be a [[Definition:Set|set]]. Then: :$X$ is [[Definition:Countable Set|countable]] {{iff}} $\size X \le \aleph_0$ where :$\size X$ denotes the [[Definition:Cardinality|cardinality]] of $X$, :$\aleph$ denotes the [[Definition:Aleph Mapping|aleph mapping]].
:$X$ is [[Definition:Countable Set|countable]] {{iff}} :there exists an [[Definition:Injection|injection]] $X \to \N$ by definition of [[Definition:Countable Set|countable set]] {{iff}} :$\size X \le \size \N$ by [[Injection iff Cardinal Inequality]] {{iff}} :$\size X \le \aleph_0$ by [[Aleph Zero equals Cardinality of...
Set is Countable iff Cardinality not greater Aleph Zero
https://proofwiki.org/wiki/Set_is_Countable_iff_Cardinality_not_greater_Aleph_Zero
https://proofwiki.org/wiki/Set_is_Countable_iff_Cardinality_not_greater_Aleph_Zero
[ "Countable Sets" ]
[ "Definition:Set", "Definition:Countable Set", "Definition:Cardinality", "Definition:Aleph Mapping" ]
[ "Definition:Countable Set", "Definition:Injection", "Definition:Countable Set", "Injection iff Cardinal Inequality", "Aleph Zero equals Cardinality of Naturals", "Category:Countable Sets" ]
proofwiki-10928
Bernoulli's Theorem
Let the probability of the occurrence of an event be $p$. Let $n$ independent trials be made, with $k$ successes. Then: :$\ds \lim_{n \mathop \to \infty} \frac k n = p$
Let the random variable $k$ have the binomial distribution with parameters $n$ and $p$, that is: :$k \sim \Binomial n p$ where $k$ denotes the number of successes of the $n$ independent trials of the event with probability $p$. From Expectation of Binomial Distribution: :$\expect k = n p \leadsto \dfrac 1 n \expect k =...
Let the [[Definition:Probability|probability]] of the [[Definition:Occurrence of Event|occurrence]] of an [[Definition:Event|event]] be $p$. Let $n$ [[Definition:Independent Events|independent trials]] be made, with $k$ [[Definition:Success|successes]]. Then: :$\ds \lim_{n \mathop \to \infty} \frac k n = p$
Let the [[Definition:Random Variable|random variable]] $k$ have the [[Definition:Binomial Distribution|binomial distribution]] with parameters $n$ and $p$, that is: :$k \sim \Binomial n p$ where $k$ denotes the number of [[Definition:Success|successes]] of the $n$ [[Definition:Independent Events|independent trials]] of...
Bernoulli's Theorem
https://proofwiki.org/wiki/Bernoulli's_Theorem
https://proofwiki.org/wiki/Bernoulli's_Theorem
[ "Bernoulli's Theorem", "Laws of Large Numbers", "Probability Theory" ]
[ "Definition:Probability", "Definition:Event/Occurrence", "Definition:Event", "Definition:Independent Events", "Definition:Bernoulli Distribution" ]
[ "Definition:Random Variable", "Definition:Binomial Distribution", "Definition:Bernoulli Distribution", "Definition:Independent Events", "Definition:Probability", "Expectation of Binomial Distribution", "Expectation is Linear", "Variance of Binomial Distribution", "Variance of Linear Combination of R...
proofwiki-10929
Time of Travel down Brachistochrone
Let a wire $AB$ be curved into the shape of a brachistochrone. Let $AB$ be embedded in a constant and uniform gravitational field where Acceleration Due to Gravity is $g$. Let a bead $P$ be released at $A$ to slide down without friction to $B$. Then the time taken for $P$ to slide from $A$ to $B$ is: :$T = \pi \sqrt {\...
That the curve $AB$ is indeed a cycloid is demonstrated in Brachistochrone is Cycloid. Let $A$ be located at the origin of a cartesian plane. We have the equations of the cycloid: {{begin-eqn}} {{eqn | l = x | r = a \paren {\theta - \sin \theta} }} {{eqn | l = y | r = a \paren {1 - \cos \theta} }} {{end-eqn...
Let a [[Definition:Wire|wire]] $AB$ be curved into the shape of a [[Definition:Brachistochrone|brachistochrone]]. Let $AB$ be embedded in a [[Definition:Constant|constant]] and [[Definition:Uniform|uniform]] [[Definition:Gravitational Field|gravitational field]] where [[Acceleration Due to Gravity]] is $g$. Let a [[D...
That the [[Definition:Curve|curve]] $AB$ is indeed a [[Definition:Cycloid|cycloid]] is demonstrated in [[Brachistochrone is Cycloid]]. Let $A$ be located at the [[Definition:Origin|origin]] of a [[Definition:Cartesian Plane|cartesian plane]]. We have the equations of the [[Definition:Cycloid|cycloid]]: {{begin-eqn}...
Time of Travel down Brachistochrone
https://proofwiki.org/wiki/Time_of_Travel_down_Brachistochrone
https://proofwiki.org/wiki/Time_of_Travel_down_Brachistochrone
[ "Cycloids" ]
[ "Definition:Wire", "Definition:Brachistochrone", "Definition:Constant", "Definition:Uniform", "Definition:Gravitational Field", "Acceleration Due to Gravity", "Definition:Bead", "Definition:Friction", "Definition:Time", "Definition:Circle/Radius", "Definition:Cycloid/Generating Circle", "Defin...
[ "Definition:Line/Curve", "Definition:Cycloid", "Brachistochrone is Cycloid", "Definition:Coordinate System/Origin", "Definition:Cartesian Plane", "Definition:Cycloid", "Definition:Derivative/Real Function/With Respect To", "Definition:Arc Distance", "Definition:Coordinate System/Origin", "Principl...
proofwiki-10930
Time of Travel down Brachistochrone/Corollary
Let a bead $P$ be released from anywhere on the wire between $A$ and $B$ to slide down without friction to $B$. Then the time taken for $P$ to slide to $B$ is: :$T = \pi \sqrt{\dfrac a g}$
That the curve $AB$ is indeed a cycloid is demonstrated in Brachistochrone is Cycloid. Let $A$ be located at the origin of a cartesian plane. Let the bead slide from an intermediate point $\theta_0$. We have: :$v = \dfrac {\d s} {\d t} = \sqrt {2 g \paren {y - y_0} }$ which leads us, via the same route as for Time of T...
Let a [[Definition:Bead|bead]] $P$ be released from anywhere on the [[Definition:Wire|wire]] between $A$ and $B$ to slide down without [[Definition:Friction|friction]] to $B$. Then the [[Definition:Time|time]] taken for $P$ to slide to $B$ is: :$T = \pi \sqrt{\dfrac a g}$
That the [[Definition:Curve|curve]] $AB$ is indeed a [[Definition:Cycloid|cycloid]] is demonstrated in [[Brachistochrone is Cycloid]]. Let $A$ be located at the [[Definition:Origin|origin]] of a [[Definition:Cartesian Plane|cartesian plane]]. Let the [[Definition:Bead|bead]] slide from an intermediate point $\theta_0...
Time of Travel down Brachistochrone/Corollary
https://proofwiki.org/wiki/Time_of_Travel_down_Brachistochrone/Corollary
https://proofwiki.org/wiki/Time_of_Travel_down_Brachistochrone/Corollary
[ "Cycloids" ]
[ "Definition:Bead", "Definition:Wire", "Definition:Friction", "Definition:Time" ]
[ "Definition:Line/Curve", "Definition:Cycloid", "Brachistochrone is Cycloid", "Definition:Coordinate System/Origin", "Definition:Cartesian Plane", "Definition:Bead", "Time of Travel down Brachistochrone", "Half Angle Formulas/Cosine", "Half Angle Formulas/Sine", "Definition:Time", "Definition:Bra...
proofwiki-10931
Rational Numbers are F-Sigma Set in Real Line
Let $\struct {\R, \tau}$ be the real number line considered asa topological space with the usual (Euclidean) topology. Then: :$\Q$ is an $F_\sigma$ set in $\struct {\R, \tau}$.
Define the set of subsets of $\R$ as: :$\FF := \set {\set x: x \in \Q}$ By Closed Real Interval is Closed Set: :$\forall x \in \Q: \closedint x x = \set x$ is closed (in topological sense) Then: :$\forall A \in \FF: A$ is closed By Cardinality of Set of Singletons: :$\card \FF = \card \Q$ where $\card \FF$ denotes the ...
Let $\struct {\R, \tau}$ be the [[Definition:Real Number Line|real number line]] considered asa [[Definition:Topological Space|topological space]] with the [[Definition:Euclidean Topology on Real Number Line|usual (Euclidean) topology]]. Then: :$\Q$ is an [[Definition:F-Sigma Set|$F_\sigma$ set]] in $\struct {\R, \ta...
Define the [[Definition:Set of Sets|set]] of [[Definition:Subset|subsets]] of $\R$ as: :$\FF := \set {\set x: x \in \Q}$ By [[Closed Real Interval is Closed Set]]: :$\forall x \in \Q: \closedint x x = \set x$ is [[Definition:Closed Set (Topology)|closed (in topological sense)]] Then: :$\forall A \in \FF: A$ is [[Defi...
Rational Numbers are F-Sigma Set in Real Line
https://proofwiki.org/wiki/Rational_Numbers_are_F-Sigma_Set_in_Real_Line
https://proofwiki.org/wiki/Rational_Numbers_are_F-Sigma_Set_in_Real_Line
[ "F-Sigma Sets" ]
[ "Definition:Real Number/Real Number Line", "Definition:Topological Space", "Definition:Euclidean Space/Euclidean Topology/Real Number Line", "Definition:F-Sigma Set" ]
[ "Definition:Set of Sets", "Definition:Subset", "Closed Real Interval is Closed Set", "Definition:Closed Set/Topology", "Definition:Closed Set/Topology", "Cardinality of Set of Singletons", "Definition:Cardinality", "Rational Numbers are Countably Infinite", "Definition:Countable Set", "Set is Coun...
proofwiki-10932
Union of Set of Singletons
Let $S$ be a set. Let $T = \set {\set x: x \in S}$ be the set of all singletons of elements of $S$. Then: :$\ds \bigcup T = S$ where $\ds \bigcup T$ denotes the union of $T$.
=== Union of $T$ Subset $S$ === Let $\ds x \in \bigcup T$. By definition of union: :$\exists A \in T: x \in A$ By definition of $T$: :$\exists y \in S: A = \set y$ Then by definition of singleton: :$x = y$ Thus $x \in S$. {{qed|lemma}}
Let $S$ be a [[Definition:Set|set]]. Let $T = \set {\set x: x \in S}$ be the [[Definition:Set|set]] of all [[Definition:Singleton|singletons]] of [[Definition:Element|elements]] of $S$. Then: :$\ds \bigcup T = S$ where $\ds \bigcup T$ denotes the [[Definition:Union of Set of Sets|union]] of $T$.
=== Union of $T$ Subset $S$ === Let $\ds x \in \bigcup T$. By definition of [[Definition:Union of Set of Sets|union]]: :$\exists A \in T: x \in A$ By definition of $T$: :$\exists y \in S: A = \set y$ Then by definition of [[Definition:Singleton|singleton]]: :$x = y$ Thus $x \in S$. {{qed|lemma}}
Union of Set of Singletons
https://proofwiki.org/wiki/Union_of_Set_of_Singletons
https://proofwiki.org/wiki/Union_of_Set_of_Singletons
[ "Set Union", "Singletons" ]
[ "Definition:Set", "Definition:Set", "Definition:Singleton", "Definition:Element", "Definition:Set Union/Set of Sets" ]
[ "Definition:Set Union/Set of Sets", "Definition:Singleton", "Definition:Singleton" ]
proofwiki-10933
Confocal Conics are Self-Orthogonal
The confocal conics defined by: :$\quad \dfrac {x^2} {a^2} + \dfrac {y^2} {a^2 - c^2} = 1$ forms a family of orthogonal trajectories which is self-orthogonal. :500px
Consider: :$(1): \quad \dfrac {x^2} {a^2} + \dfrac {y^2} {a^2 - c^2} = 1$ From Equation of Confocal Ellipses: Formulation 2: :$(1)$ defines an ellipse when $a^2 > c^2$. From Equation of Confocal Hyperbolas: Formulation 2: :$(1)$ defines a hyperbola when $a^2 < c^2$. Thus it is seen that $(1)$ is that of a conic section...
The [[Definition:Confocal Conics|confocal conics]] defined by: :$\quad \dfrac {x^2} {a^2} + \dfrac {y^2} {a^2 - c^2} = 1$ forms a [[Definition:Orthogonal Trajectories|family of orthogonal trajectories]] which is [[Definition:Self-Orthogonal Trajectories|self-orthogonal]]. :[[File:ConfocalConics.png|500px]]
Consider: :$(1): \quad \dfrac {x^2} {a^2} + \dfrac {y^2} {a^2 - c^2} = 1$ From [[Equation of Confocal Ellipses/Formulation 2|Equation of Confocal Ellipses: Formulation 2]]: :$(1)$ defines an [[Definition:Ellipse|ellipse]] when $a^2 > c^2$. From [[Equation of Confocal Hyperbolas/Formulation 2|Equation of Confocal Hype...
Confocal Conics are Self-Orthogonal
https://proofwiki.org/wiki/Confocal_Conics_are_Self-Orthogonal
https://proofwiki.org/wiki/Confocal_Conics_are_Self-Orthogonal
[ "Orthogonal Trajectories", "Conic Sections", "Orthogonal Curves" ]
[ "Definition:Confocal Conics", "Definition:Orthogonal Trajectories", "Definition:Self-Orthogonal Trajectories", "File:ConfocalConics.png" ]
[ "Equation of Confocal Ellipses/Formulation 2", "Definition:Ellipse", "Equation of Confocal Hyperbolas/Formulation 2", "Definition:Hyperbola", "Definition:Conic Section", "Definition:Formation of Ordinary Differential Equation by Elimination", "Definition:Differentiation", "Definition:Self-Orthogonal T...
proofwiki-10934
T1 Space is T1/2 Space
Let $T$ be a $T_1$ topological space. Then $T$ is $T_{\frac 1 2}$ space.
By Closure of Derivative is Derivative in T1 Space: :$\forall A \subseteq T: \paren {A'}^- = A'$ where :$A'$ denotes the derivative of $A$ :$\paren {A'}^-$ denotes the closure of $A'$ Then by Topological Closure is Closed: :$\forall A \subseteq T: A'$ is closed Thus by definition: :$T$ is $T_{\frac 1 2}$ space {{qed}}
Let $T$ be a [[Definition:T1 Space|$T_1$]] [[Definition:Topological Space|topological space]]. Then $T$ is [[Definition:T1/2 Space|$T_{\frac 1 2}$ space]].
By [[Closure of Derivative is Derivative in T1 Space]]: :$\forall A \subseteq T: \paren {A'}^- = A'$ where :$A'$ denotes the [[Definition:Set Derivative|derivative]] of $A$ :$\paren {A'}^-$ denotes the [[Definition:Closure (Topology)|closure]] of $A'$ Then by [[Topological Closure is Closed]]: :$\forall A \subseteq T:...
T1 Space is T1/2 Space
https://proofwiki.org/wiki/T1_Space_is_T1/2_Space
https://proofwiki.org/wiki/T1_Space_is_T1/2_Space
[ "T1 Spaces", "T1/2 Spaces" ]
[ "Definition:T1 Space", "Definition:Topological Space", "Definition:T1/2 Space" ]
[ "Closure of Derivative is Derivative in T1 Space", "Definition:Set Derivative", "Definition:Closure (Topology)", "Topological Closure is Closed", "Definition:Closed Set/Topology", "Definition:T1/2 Space" ]
proofwiki-10935
T1/2 Space is T0 Space
Let $T = \struct {S, \tau}$ be a $T_{\frac 1 2}$ topological space. Then $T$ is $T_0$ space.
By Characterization of T0 Space by Closures of Singletons it suffices to prove that :$\forall x, y \in S: x \ne y \implies x \notin \set y^- \lor y \notin \set x^-$ where $\set y^-$ denotes the closure of $\set y$. Let $x, y$ be points of $T$ such that: :$x \ne y$ {{AimForCont}}: :$x \in \set y^- \land y \in \set x^-$ ...
Let $T = \struct {S, \tau}$ be a [[Definition:T1/2 Space|$T_{\frac 1 2}$ topological space]]. Then $T$ is [[Definition:T0 Space|$T_0$ space]].
By [[Characterization of T0 Space by Closures of Singletons]] it suffices to prove that :$\forall x, y \in S: x \ne y \implies x \notin \set y^- \lor y \notin \set x^-$ where $\set y^-$ denotes the [[Definition:Closure (Topology)|closure]] of $\set y$. Let $x, y$ be [[Definition:Element|points]] of $T$ such that: :$x ...
T1/2 Space is T0 Space
https://proofwiki.org/wiki/T1/2_Space_is_T0_Space
https://proofwiki.org/wiki/T1/2_Space_is_T0_Space
[ "T0 Spaces", "T1/2 Spaces" ]
[ "Definition:T1/2 Space", "Definition:T0 Space" ]
[ "Characterization of T0 Space by Closures of Singletons", "Definition:Closure (Topology)", "Definition:Element", "Definition:Set Derivative", "Definition:Open Set/Topology", "Definition:Topological Space", "Characterization of Derivative by Open Sets", "Definition:Set Intersection", "Definition:Sing...
proofwiki-10936
Parabolas Inscribed in Shared Tangent Lines
Let the function $\map f x = A x^2 + B x + C_1$ be a curve embedded in the Euclidean Plane. Let $\map {y_1} x$ be the equation of the tangent line at $\tuple {Q, \map f Q}$ on $f$. Let $\map {y_2} x$ be the equation of the tangent line at $\tuple {-Q, \map f {-Q} }$ on $f$. Then there exists another function $\map g x$...
The tangent line at $\tuple {Q, \map f \Q}$ on $f$ is defined as: :$\map {y_1} x = \paren {2 A Q + B} x + b_1$ where $2 A Q + B$ is the slope of the tangent line on the point $\tuple {Q, \map g Q}$ on $f$. Substitute in the coordinates of the point $\tuple {Q, \map g Q}$ to $y_1$ and solve for $b_1$. This will reveal t...
Let the function $\map f x = A x^2 + B x + C_1$ be a curve embedded in the [[Definition:Euclidean Plane|Euclidean Plane]]. Let $\map {y_1} x$ be the equation of the [[Definition:Tangent Line|tangent line]] at $\tuple {Q, \map f Q}$ on $f$. Let $\map {y_2} x$ be the equation of the [[Definition:Tangent Line|tangent li...
The [[Definition:Tangent Line|tangent line]] at $\tuple {Q, \map f \Q}$ on $f$ is defined as: :$\map {y_1} x = \paren {2 A Q + B} x + b_1$ where $2 A Q + B$ is the [[Definition:Slope of Straight Line|slope]] of the [[Definition:Tangent Line|tangent line]] on the point $\tuple {Q, \map g Q}$ on $f$. Substitute in t...
Parabolas Inscribed in Shared Tangent Lines
https://proofwiki.org/wiki/Parabolas_Inscribed_in_Shared_Tangent_Lines
https://proofwiki.org/wiki/Parabolas_Inscribed_in_Shared_Tangent_Lines
[ "Analytic Geometry", "Tangents" ]
[ "Definition:Euclidean Plane", "Definition:Tangent Line", "Definition:Tangent Line", "Definition:Euclidean Plane", "Definition:Tangent Line", "Definition:Tangent Line", "Definition:Tangent Line", "Definition:Tangent Line" ]
[ "Definition:Tangent Line", "Definition:Slope/Straight Line", "Definition:Tangent Line", "Definition:Coordinate System", "Definition:Slope/Straight Line", "Definition:Tangent Line", "Definition:Coordinate System", "Definition:Intercept/Y-Intercept", "Definition:Intercept/Y-Intercept", "Definition:D...
proofwiki-10937
Characterization of T0 Space by Closures of Singletons
Let $T = \struct {S, \tau}$ be a topological space. Then :$T$ is a $T_0$ space {{iff}}: ::$\forall x, y \in S: x \ne y \implies x \notin \set y^- \lor y \notin \set x^-$ where $\set y^-$ denotes the closure of $\set y$.
=== Sufficient Condition === Let $T$ be a $T_0$ space. Let $x, y \in S$ such that :$x \ne y$ {{AimForCont}} :$x \in \set y^- \land y \in \set x^-$ Then: {{begin-eqn}} {{eqn | l = x | o = \in | r = \set y^- }} {{eqn | lo= \land | l = \set y | o = \subseteq | r = \set x^- }} {{eqn | ll= \lea...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Then :$T$ is a [[Definition:T0 Space|$T_0$ space]] {{iff}}: ::$\forall x, y \in S: x \ne y \implies x \notin \set y^- \lor y \notin \set x^-$ where $\set y^-$ denotes the [[Definition:Closure (Topology)|closure]] of $\set y$.
=== Sufficient Condition === Let $T$ be a [[Definition:T0 Space|$T_0$ space]]. Let $x, y \in S$ such that :$x \ne y$ {{AimForCont}} :$x \in \set y^- \land y \in \set x^-$ Then: {{begin-eqn}} {{eqn | l = x | o = \in | r = \set y^- }} {{eqn | lo= \land | l = \set y | o = \subseteq | r =...
Characterization of T0 Space by Closures of Singletons
https://proofwiki.org/wiki/Characterization_of_T0_Space_by_Closures_of_Singletons
https://proofwiki.org/wiki/Characterization_of_T0_Space_by_Closures_of_Singletons
[ "T0 Spaces" ]
[ "Definition:Topological Space", "Definition:T0 Space", "Definition:Closure (Topology)" ]
[ "Definition:T0 Space", "Topological Closure of Subset is Subset of Topological Closure", "Closure of Topological Closure equals Closure", "Characterization of T0 Space by Distinct Closures of Singletons", "Proof by Contradiction", "Characterization of T0 Space by Distinct Closures of Singletons", "Proof...
proofwiki-10938
Characterization of T0 Space by Distinct Closures of Singletons
Let $T = \struct {S, \tau}$ be a topological space. Then :$T$ is a $T_0$ space {{iff}} ::$\forall x, y \in S: x \ne y \implies \set x^- \ne \set y^-$ where $\set y^-$ denotes the closure of $\set y$.
=== Sufficient Condition === Let $T$ be a $T_0$ space. Let $x, y \in S$ such that :$x \ne y$ By definition of $T_0$ space: :$\paren {\exists U \in \tau: x \in U \land y \notin U} \lor \paren {\exists U \in \tau: x \notin U \land y \in U}$ {{WLOG}}, suppose :$\exists U \in \tau: x \in U \land y \notin U$ By definition o...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Then :$T$ is a [[Definition:T0 Space|$T_0$ space]] {{iff}} ::$\forall x, y \in S: x \ne y \implies \set x^- \ne \set y^-$ where $\set y^-$ denotes the [[Definition:Closure (Topology)|closure]] of $\set y$.
=== Sufficient Condition === Let $T$ be a [[Definition:T0 Space|$T_0$ space]]. Let $x, y \in S$ such that :$x \ne y$ By definition of [[Definition:T0 Space|$T_0$ space]]: :$\paren {\exists U \in \tau: x \in U \land y \notin U} \lor \paren {\exists U \in \tau: x \notin U \land y \in U}$ {{WLOG}}, suppose :$\exists U...
Characterization of T0 Space by Distinct Closures of Singletons
https://proofwiki.org/wiki/Characterization_of_T0_Space_by_Distinct_Closures_of_Singletons
https://proofwiki.org/wiki/Characterization_of_T0_Space_by_Distinct_Closures_of_Singletons
[ "T0 Spaces" ]
[ "Definition:Topological Space", "Definition:T0 Space", "Definition:Closure (Topology)" ]
[ "Definition:T0 Space", "Definition:T0 Space", "Definition:Singleton", "Set is Subset of its Topological Closure", "Definition:Subset", "Definition:Set Intersection", "Definition:Singleton", "Definition:Set Intersection", "Open Set Disjoint from Set is Disjoint from Closure", "Definition:Singleton"...
proofwiki-10939
Characterization of T0 Space by Closed Sets
Let $T = \struct {S, \tau}$ be a topological space. Then :$T$ is a $T_0$ space {{iff}} ::for every points $x, y \in S$ if $x \ne y$ then :::there exists a closed subset $F$ of $S$ such that $x \in F$ and $y \notin F$ ::or :::there exists a closed subset $F$ of $S$ such that $x \notin F$ and $y \in F$
=== Sufficient Condition === Let $T$ be a $T_0$ space. Let $x, y \in S$ such that :$x \ne y$ By definition of $T_0$ space: :$\paren {\exists U \in \tau: x \in U \land y \notin U} \lor \paren {\exists U \in \tau: x \notin U \land y \in U}$ {{WLOG}}, suppose: :$\exists U \in \tau: x \in U \land y \notin U$ By definition:...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Then :$T$ is a [[Definition:T0 Space|$T_0$ space]] {{iff}} ::for every [[Definition:Element|points]] $x, y \in S$ if $x \ne y$ then :::there exists a [[Definition:Closed Set (Topology)|closed]] [[Definition:Subset|subset]] $F$ of $S$ ...
=== Sufficient Condition === Let $T$ be a [[Definition:T0 Space|$T_0$ space]]. Let $x, y \in S$ such that :$x \ne y$ By definition of [[Definition:T0 Space|$T_0$ space]]: :$\paren {\exists U \in \tau: x \in U \land y \notin U} \lor \paren {\exists U \in \tau: x \notin U \land y \in U}$ {{WLOG}}, suppose: :$\exists ...
Characterization of T0 Space by Closed Sets
https://proofwiki.org/wiki/Characterization_of_T0_Space_by_Closed_Sets
https://proofwiki.org/wiki/Characterization_of_T0_Space_by_Closed_Sets
[ "T0 Spaces" ]
[ "Definition:Topological Space", "Definition:T0 Space", "Definition:Element", "Definition:Closed Set/Topology", "Definition:Subset", "Definition:Closed Set/Topology", "Definition:Subset" ]
[ "Definition:T0 Space", "Definition:T0 Space", "Definition:Closed Set/Topology", "Definition:Relative Complement", "Definition:Relative Complement", "Definition:Closed Set/Topology" ]
proofwiki-10940
Linear Eccentricity of Ellipse from Major and Minor Axis
Let $K$ be an ellipse whose major axis is $2 a$ and whose minor axis is $2 b$. Let $c$ be the linear eccentricity of $K$. Then: :$a^2 = b^2 + c^2$
:500px Let the foci of $K$ be $F_1$ and $F_2$. Let the vertices of $K$ be $V_1$ and $V_2$. Let the covertices of $K$ be $C_1$ and $C_2$. Let $P = \tuple {x, y}$ be an arbitrary point on the locus of $K$. From the equidistance property of $K$ we have that: :$F_1 P + F_2 P = d$ where $d$ is a constant for this particular...
Let $K$ be an [[Definition:Ellipse|ellipse]] whose [[Definition:Major Axis of Ellipse|major axis]] is $2 a$ and whose [[Definition:Minor Axis of Ellipse|minor axis]] is $2 b$. Let $c$ be the [[Definition:Linear Eccentricity|linear eccentricity]] of $K$. Then: :$a^2 = b^2 + c^2$
:[[File:EllipseFocus MajorMinorAxes.png|500px]] Let the [[Definition:Focus of Ellipse|foci]] of $K$ be $F_1$ and $F_2$. Let the [[Definition:Vertex of Ellipse|vertices]] of $K$ be $V_1$ and $V_2$. Let the [[Definition:Covertex of Ellipse|covertices]] of $K$ be $C_1$ and $C_2$. Let $P = \tuple {x, y}$ be an arbitr...
Linear Eccentricity of Ellipse from Major and Minor Axis
https://proofwiki.org/wiki/Linear_Eccentricity_of_Ellipse_from_Major_and_Minor_Axis
https://proofwiki.org/wiki/Linear_Eccentricity_of_Ellipse_from_Major_and_Minor_Axis
[ "Linear Eccentricity of Ellipse from Major and Minor Axis", "Linear Eccentricity", "Major Axis of Ellipse", "Minor Axis of Ellipse", "Ellipses" ]
[ "Definition:Ellipse", "Definition:Ellipse/Major Axis", "Definition:Ellipse/Minor Axis", "Definition:Linear Eccentricity" ]
[ "File:EllipseFocus MajorMinorAxes.png", "Definition:Ellipse/Focus", "Definition:Ellipse/Vertex", "Definition:Ellipse/Covertex", "Definition:Point", "Definition:Locus", "Definition:Ellipse/Equidistance", "Definition:Constant", "Definition:Ellipse", "Definition:Point", "Pythagoras's Theorem", "P...
proofwiki-10941
Equidistance of Ellipse equals Major Axis
Let $K$ be an ellipse whose foci are $F_1$ and $F_2$. Let $P$ be an arbitrary point on $K$. Let $d$ be the constant distance such that: :$d_1 + d_2 = d$ where: :$d_1 = P F_1$ :$d_2 = P F_2$ Then $d$ is equal to the major axis of $K$.
:400px By the equidistance property of $K$: :$d_1 + d_2 = d$ applies to all points $P$ on $K$. Thus it also applies to the two vertices $V_1$ and $V_2$: :$V_1 F_1 + V_1 F_2 = d$ :$V_2 F_1 + V_2 F_2 = d$ Adding: :$V_1 F_1 + V_2 F_1 + V_1 F_2 + V_2 F_2 = 2 d$ But: :$V_1 F_1 + V_2 F_1 = V_1 V_2$ :$V_1 F_2 + V_2 F_2 = V_1 ...
Let $K$ be an [[Definition:Ellipse|ellipse]] whose [[Definition:Focus of Ellipse|foci]] are $F_1$ and $F_2$. Let $P$ be an arbitrary [[Definition:Point|point]] on $K$. Let $d$ be the [[Definition:Constant|constant]] [[Definition:Distance between Points|distance]] such that: :$d_1 + d_2 = d$ where: :$d_1 = P F_1$ :$d...
:[[File:EllipseEquidistanceMajorAxis.png|400px]] By the [[Definition:Equidistance Property of Ellipse|equidistance property]] of $K$: :$d_1 + d_2 = d$ applies to all [[Definition:Point|points]] $P$ on $K$. Thus it also applies to the two [[Definition:Vertex of Ellipse|vertices]] $V_1$ and $V_2$: :$V_1 F_1 + V_1 F_2...
Equidistance of Ellipse equals Major Axis
https://proofwiki.org/wiki/Equidistance_of_Ellipse_equals_Major_Axis
https://proofwiki.org/wiki/Equidistance_of_Ellipse_equals_Major_Axis
[ "Ellipses" ]
[ "Definition:Ellipse", "Definition:Ellipse/Focus", "Definition:Point", "Definition:Constant", "Definition:Distance between Points", "Definition:Ellipse/Major Axis" ]
[ "File:EllipseEquidistanceMajorAxis.png", "Definition:Ellipse/Equidistance", "Definition:Point", "Definition:Ellipse/Vertex", "Definition:Ellipse/Major Axis" ]
proofwiki-10942
Equidistance of Hyperbola equals Transverse Axis
Let $K$ be an hyperbola whose foci are $F_1$ and $F_2$. Let $P$ be an arbitrary point on $K$. Let $d$ be the constant distance such that: :$\size {d_1 - d_2} = d$ where: :$d_1 = P F_1$ :$d_2 = P F_2$ Then $d$ is equal to the transverse axis of $K$.
&nbsp; :400px By the equidistance property of $K$: :$\size {d_1 - d_2} = d$ applies to all points $P$ on $K$. Thus it also applies to the two vertices $V_1$ and $V_2$. Observing the signs of $\size {d_1 - d_2}$ as appropriate: :$V_1 F_2 - V_1 F_1 = d$ :$V_2 F_1 - V_2 F_2 = d$ Adding: :$\paren {V_1 F_2 - V_2 F_2} + \par...
Let $K$ be an [[Definition:Hyperbola|hyperbola]] whose [[Definition:Focus of Hyperbola|foci]] are $F_1$ and $F_2$. Let $P$ be an arbitrary [[Definition:Point|point]] on $K$. Let $d$ be the [[Definition:Constant|constant]] [[Definition:Distance between Points|distance]] such that: :$\size {d_1 - d_2} = d$ where: :$d_...
&nbsp; :[[File:HyperbolaEquidistanceTransverseAxis.png|400px]] By the [[Definition:Equidistance Property of Hyperbola|equidistance property]] of $K$: :$\size {d_1 - d_2} = d$ applies to all [[Definition:Point|points]] $P$ on $K$. Thus it also applies to the two [[Definition:Vertex of Hyperbola|vertices]] $V_1$ and...
Equidistance of Hyperbola equals Transverse Axis
https://proofwiki.org/wiki/Equidistance_of_Hyperbola_equals_Transverse_Axis
https://proofwiki.org/wiki/Equidistance_of_Hyperbola_equals_Transverse_Axis
[ "Hyperbolas" ]
[ "Definition:Hyperbola", "Definition:Hyperbola/Focus", "Definition:Point", "Definition:Constant", "Definition:Distance between Points", "Definition:Hyperbola/Transverse Axis" ]
[ "File:HyperbolaEquidistanceTransverseAxis.png", "Definition:Hyperbola/Equidistance", "Definition:Point", "Definition:Hyperbola/Vertex", "Definition:Hyperbola/Transverse Axis", "Category:Hyperbolas" ]
proofwiki-10943
Equivalence of Definitions of Ellipse
The following definitions of an ellipse are equivalent:
Let $K$ be an ellipse aligned in a cartesian plane in reduced form. Thus its foci are at $\tuple {\mathop \pm c, 0}$. Let: :the major axis of $K$ have length $2 a$ :the minor axis of $K$ have length $2 b$. From Equation of Ellipse in Reduced Form, the equation of $K$ is: :$\dfrac {x^2} {a^2} + \dfrac {y^2} {b^2} = 1$ T...
The following definitions of an [[Definition:Ellipse|ellipse]] are [[Definition:Logical Equivalence|equivalent]]:
Let $K$ be an [[Definition:Ellipse|ellipse]] aligned in a [[Definition:Cartesian Plane|cartesian plane]] in [[Definition:Reduced Form of Ellipse|reduced form]]. Thus its [[Definition:Focus of Ellipse|foci]] are at $\tuple {\mathop \pm c, 0}$. Let: :the [[Definition:Major Axis of Ellipse|major axis]] of $K$ have [[De...
Equivalence of Definitions of Ellipse
https://proofwiki.org/wiki/Equivalence_of_Definitions_of_Ellipse
https://proofwiki.org/wiki/Equivalence_of_Definitions_of_Ellipse
[ "Ellipses" ]
[ "Definition:Ellipse", "Definition:Logical Equivalence" ]
[ "Definition:Ellipse", "Definition:Cartesian Plane", "Definition:Conic Section/Reduced Form/Ellipse", "Definition:Ellipse/Focus", "Definition:Ellipse/Major Axis", "Definition:Linear Measure/Length", "Definition:Ellipse/Minor Axis", "Definition:Linear Measure/Length", "Equation of Ellipse in Reduced F...
proofwiki-10944
Focus of Hyperbola from Transverse and Conjugate Axis
Let $K$ be a hyperbola whose transverse axis is $2 a$ and whose conjugate axis is $2 b$. Let $c$ be the distance of the foci of $K$ from the center. Then: :$c^2 = a^2 + b^2$
&nbsp; :500px Let the foci of $K$ be $F_1$ and $F_2$. Let the vertices of $K$ be $V_1$ and $V_2$. Let the covertices of $K$ be $C_1$ and $C_2$. Let $P = \tuple {x, y}$ be an arbitrary point on the locus of $K$. From the equidistance property of $K$ we have that: :$\size {F_1 P - F_2 P} = d$ where $d$ is a constant for ...
Let $K$ be a [[Definition:Hyperbola|hyperbola]] whose [[Definition:Transverse Axis of Hyperbola|transverse axis]] is $2 a$ and whose [[Definition:Conjugate Axis of Hyperbola|conjugate axis]] is $2 b$. Let $c$ be the [[Definition:Distance between Points|distance]] of the [[Definition:Focus of Hyperbola|foci]] of $K$ fr...
&nbsp; :[[File:HyperbolaFocusTransConj.png|500px]] Let the [[Definition:Focus of Hyperbola|foci]] of $K$ be $F_1$ and $F_2$. Let the [[Definition:Vertex of Hyperbola|vertices]] of $K$ be $V_1$ and $V_2$. Let the [[Definition:Covertex of Hyperbola|covertices]] of $K$ be $C_1$ and $C_2$. Let $P = \tuple {x, y}$ be...
Focus of Hyperbola from Transverse and Conjugate Axis
https://proofwiki.org/wiki/Focus_of_Hyperbola_from_Transverse_and_Conjugate_Axis
https://proofwiki.org/wiki/Focus_of_Hyperbola_from_Transverse_and_Conjugate_Axis
[ "Hyperbolas" ]
[ "Definition:Hyperbola", "Definition:Hyperbola/Transverse Axis", "Definition:Hyperbola/Conjugate Axis", "Definition:Distance between Points", "Definition:Hyperbola/Focus", "Definition:Ellipse/Center" ]
[ "File:HyperbolaFocusTransConj.png", "Definition:Hyperbola/Focus", "Definition:Hyperbola/Vertex", "Definition:Hyperbola/Covertex", "Definition:Point", "Definition:Locus", "Definition:Hyperbola/Equidistance", "Definition:Constant", "Definition:Hyperbola", "Definition:Point", "Category:Hyperbolas" ...
proofwiki-10945
Equation of Hyperbola in Reduced Form/Cartesian Frame/Parametric Form 1
The right-hand branch of $K$ can be expressed in parametric form as: :$\begin {cases} x = a \cosh \theta \\ y = b \sinh \theta \end {cases}$
Let the point $\tuple {x, y}$ satisfy the equations: {{begin-eqn}} {{eqn | l = x | r = a \cosh \theta }} {{eqn | l = y | r = b \sinh \theta }} {{end-eqn}} Then: {{begin-eqn}} {{eqn | l = \frac {x^2} {a^2} - \frac {y^2} {b^2} | r = \frac {\paren {a \cosh \theta}^2} {a^2} - \frac {\paren {b \sinh \theta...
The right-hand [[Definition:Branch of Hyperbola|branch]] of $K$ can be expressed in [[Definition:Parametric Equation|parametric form]] as: :$\begin {cases} x = a \cosh \theta \\ y = b \sinh \theta \end {cases}$
Let the point $\tuple {x, y}$ satisfy the equations: {{begin-eqn}} {{eqn | l = x | r = a \cosh \theta }} {{eqn | l = y | r = b \sinh \theta }} {{end-eqn}} Then: {{begin-eqn}} {{eqn | l = \frac {x^2} {a^2} - \frac {y^2} {b^2} | r = \frac {\paren {a \cosh \theta}^2} {a^2} - \frac {\paren {b \sinh \t...
Equation of Hyperbola in Reduced Form/Cartesian Frame/Parametric Form 1
https://proofwiki.org/wiki/Equation_of_Hyperbola_in_Reduced_Form/Cartesian_Frame/Parametric_Form_1
https://proofwiki.org/wiki/Equation_of_Hyperbola_in_Reduced_Form/Cartesian_Frame/Parametric_Form_1
[ "Equation of Hyperbola in Reduced Form" ]
[ "Definition:Hyperbola/Branch", "Definition:Parametric Equation" ]
[ "Difference of Squares of Hyperbolic Cosine and Sine" ]
proofwiki-10946
Set of Condensation Points is Subset of Derivative
Let $T = \left({S, \tau}\right)$ be a topological space. Let $A$ be a subset of $S$. Then: :$A^0 \subseteq A'$ where :$A^0$ denotes the set of condensation points of $A$ :$A'$ denotes the derivative of $A$
Let $x \in A^0$. By definition of set of condensation points: :$x$ is condensation point of $A$ By definition of condensation point: :$x$ is limit point of $A$ By definition of derived set: :$x \in A'$ {{qed}}
Let $T = \left({S, \tau}\right)$ be a [[Definition:Topological Space|topological space]]. Let $A$ be a [[Definition:Subset|subset]] of $S$. Then: :$A^0 \subseteq A'$ where :$A^0$ denotes the [[Definition:Set of Condensation Points|set of condensation points]] of $A$ :$A'$ denotes the [[Definition:Set Derivative|deri...
Let $x \in A^0$. By definition of [[Definition:Set of Condensation Points|set of condensation points]]: :$x$ is [[Definition:Condensation Point|condensation point]] of $A$ By definition of [[Definition:Condensation Point|condensation point]]: :$x$ is [[Definition:Limit Point of Set|limit point]] of $A$ By definition...
Set of Condensation Points is Subset of Derivative
https://proofwiki.org/wiki/Set_of_Condensation_Points_is_Subset_of_Derivative
https://proofwiki.org/wiki/Set_of_Condensation_Points_is_Subset_of_Derivative
[ "Condensation Points", "Set Derivatives" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Set of Condensation Points", "Definition:Set Derivative" ]
[ "Definition:Set of Condensation Points", "Definition:Condensation Point", "Definition:Condensation Point", "Definition:Limit Point/Topology/Set", "Definition:Derived Set" ]
proofwiki-10947
Closure of Set of Condensation Points equals Itself
Let $T = \struct {S, \tau}$ be a topological space. Let $A$ be a subset of $S$. Then: :$\paren {A^0}^- = A^0$ where :$A^0$ denotes the set of condensation points of $A$ :$A^-$ denotes the closure of $A$
By Set is Subset of its Topological Closure: :$A^0 \subseteq \paren {A^0}^-$ To prove the equality by definition of set equality it suffices to show the inclusion: :$\paren {A^0}^- \subseteq A^0$ Let $x \in \paren {A^0}^-$. We will prove that :$(1): \quad \forall U \in \tau: x \in U \implies A \cap U$ is uncountable Le...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Let $A$ be a [[Definition:Subset|subset]] of $S$. Then: :$\paren {A^0}^- = A^0$ where :$A^0$ denotes the [[Definition:Set of Condensation Points|set of condensation points]] of $A$ :$A^-$ denotes the [[Definition:Closure (Topology)|...
By [[Set is Subset of its Topological Closure]]: :$A^0 \subseteq \paren {A^0}^-$ To prove the equality by definition of [[Definition:Set Equality|set equality]] it suffices to show the inclusion: :$\paren {A^0}^- \subseteq A^0$ Let $x \in \paren {A^0}^-$. We will prove that :$(1): \quad \forall U \in \tau: x \in U \...
Closure of Set of Condensation Points equals Itself
https://proofwiki.org/wiki/Closure_of_Set_of_Condensation_Points_equals_Itself
https://proofwiki.org/wiki/Closure_of_Set_of_Condensation_Points_equals_Itself
[ "Condensation Points", "Set Closures" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Set of Condensation Points", "Definition:Closure (Topology)" ]
[ "Set is Subset of its Topological Closure", "Definition:Set Equality", "Definition:Countable Set", "Definition:Open Set/Topology", "Definition:Subset", "Condition for Point being in Closure", "Definition:Empty Set", "Definition:Set Intersection", "Definition:Set of Condensation Points", "Definitio...
proofwiki-10948
First Order ODE/(x + y) dx = (x - y) dy
is a homogeneous differential equation with general solution: :$\arctan \dfrac y x = \ln \sqrt {x^2 + y^2} + C$
Let: :$\map M {x, y} = x + y$ :$\map N {x, y} = x - y$ We have that: :$\map M {t x, t y} = t x + t y = t \paren {x + y} = t \map M {x, y}$ :$\map N {t x, t y} = t x - t y = t \paren {x - y} = t \map N {x, y}$ Thus both $M$ and $N$ are homogeneous functions of degree $1$. Thus by definition $(1)$ is a homogeneous di...
is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|general solution]]: :$\arctan \dfrac y x = \ln \sqrt {x^2 + y^2} + C$
Let: :$\map M {x, y} = x + y$ :$\map N {x, y} = x - y$ We have that: :$\map M {t x, t y} = t x + t y = t \paren {x + y} = t \map M {x, y}$ :$\map N {t x, t y} = t x - t y = t \paren {x - y} = t \map N {x, y}$ Thus both $M$ and $N$ are [[Definition:Homogeneous Real Function|homogeneous functions]] of [[Definition...
First Order ODE/(x + y) dx = (x - y) dy/Proof 1
https://proofwiki.org/wiki/First_Order_ODE/(x_+_y)_dx_=_(x_-_y)_dy
https://proofwiki.org/wiki/First_Order_ODE/(x_+_y)_dx_=_(x_-_y)_dy/Proof_1
[ "Examples of First Order ODEs", "Examples of Homogeneous Differential Equation", "First Order ODE/(x + y) dx = (x - y) dy" ]
[ "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Homogeneous Differential Equation", "Definition:Fraction/Numerator", "Definition:Fraction/Denominator", "Solution to Homogeneous Differential Equation", "Primitive of Reciprocal of x squared pl...
proofwiki-10949
First Order ODE/(x + y) dx = (x - y) dy
is a homogeneous differential equation with general solution: :$\arctan \dfrac y x = \ln \sqrt {x^2 + y^2} + C$
We have: {{begin-eqn}} {{eqn | l = \paren {x + y} \rd x | r = \paren {x - y} \rd y | c = }} {{eqn | ll= \leadsto | l = x \rd y - y \rd x | r = x \rd x + y \rd y | c = rearranging }} {{eqn | ll= \leadsto | l = \frac {x \rd y - y \rd x} {x^2 + y^2} | r = \frac {x \rd x + y \rd y...
is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|general solution]]: :$\arctan \dfrac y x = \ln \sqrt {x^2 + y^2} + C$
We have: {{begin-eqn}} {{eqn | l = \paren {x + y} \rd x | r = \paren {x - y} \rd y | c = }} {{eqn | ll= \leadsto | l = x \rd y - y \rd x | r = x \rd x + y \rd y | c = rearranging }} {{eqn | ll= \leadsto | l = \frac {x \rd y - y \rd x} {x^2 + y^2} | r = \frac {x \rd x + y \rd y...
First Order ODE/(x + y) dx = (x - y) dy/Proof 2
https://proofwiki.org/wiki/First_Order_ODE/(x_+_y)_dx_=_(x_-_y)_dy
https://proofwiki.org/wiki/First_Order_ODE/(x_+_y)_dx_=_(x_-_y)_dy/Proof_2
[ "Examples of First Order ODEs", "Examples of Homogeneous Differential Equation", "First Order ODE/(x + y) dx = (x - y) dy" ]
[ "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Differential of Sum of Squares", "Differential of Arctangent of Quotient" ]
proofwiki-10950
First Order ODE/(x^2 - 2 y^2) dx + x y dy = 0
is a homogeneous differential equation with solution: :$y^2 = x^2 + C x^4$
$(1)$ can also be rendered: :$\dfrac {\d y} {\d x} = -\dfrac {x^2 - 2 y^2} {x y}$ Let: :$\map M {x, y} = x^2 - 2 y^2$ :$\map N {x, y} = x y$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = \paren {t x}^2 - 2 \paren {t y}^2 | c = }} {{eqn | r = t^2 \paren {x^2 - 2 y^2} | c...
is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$y^2 = x^2 + C x^4$
$(1)$ can also be rendered: :$\dfrac {\d y} {\d x} = -\dfrac {x^2 - 2 y^2} {x y}$ Let: :$\map M {x, y} = x^2 - 2 y^2$ :$\map N {x, y} = x y$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = \paren {t x}^2 - 2 \paren {t y}^2 | c = }} {{eqn | r = t^2 \paren {x^2 - 2 y^2} ...
First Order ODE/(x^2 - 2 y^2) dx + x y dy = 0
https://proofwiki.org/wiki/First_Order_ODE/(x^2_-_2_y^2)_dx_+_x_y_dy_=_0
https://proofwiki.org/wiki/First_Order_ODE/(x^2_-_2_y^2)_dx_+_x_y_dy_=_0
[ "Examples of Homogeneous Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Homogeneous Differential Equation", "Solution to Homogeneous Differential Equation", "Primitive of x over x squared minus a squared" ]
proofwiki-10951
First Order ODE/x^2 y' - 3 x y - 2 y^2 = 0
is a homogeneous differential equation with solution: :$y = C x^2 \paren {x + y}$
Let: :$\map M {x, y} = 3 x y + 2 y^2$ :$\map N {x, y} = x^2$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = 3 t x t y + 2 \paren {t y}^2 | c = }} {{eqn | r = t^2 \paren {3 x y + 2 y^2} | c = }} {{eqn | r = t^2 \, \map M {x, y} | c = }} {{end-eqn}} {{begin-eqn}} {...
is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$y = C x^2 \paren {x + y}$
Let: :$\map M {x, y} = 3 x y + 2 y^2$ :$\map N {x, y} = x^2$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = 3 t x t y + 2 \paren {t y}^2 | c = }} {{eqn | r = t^2 \paren {3 x y + 2 y^2} | c = }} {{eqn | r = t^2 \, \map M {x, y} | c = }} {{end-eqn}} {{begin-eqn...
First Order ODE/x^2 y' - 3 x y - 2 y^2 = 0
https://proofwiki.org/wiki/First_Order_ODE/x^2_y'_-_3_x_y_-_2_y^2_=_0
https://proofwiki.org/wiki/First_Order_ODE/x^2_y'_-_3_x_y_-_2_y^2_=_0
[ "Examples of Homogeneous Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Homogeneous Differential Equation", "Solution to Homogeneous Differential Equation", "Primitive of Reciprocal of x by a x + b" ]
proofwiki-10952
Set of Condensation Points is Monotone
Let $T = \struct {S, \tau}$ be a topological space. Let $A, B$ be subsets of $S$. Then: :$A \subseteq B \implies {A^0} \subseteq B^0$ where :$A^0$ denotes the set of condensation points of $A$
Assume :$A \subseteq B$ Let $x \in A^0$. By definition of set of condensation points: :$x$ is condensation point of $A$ By definition of condensation point: :$x$ is limit point of $A$ such that $\forall U \in \tau: A \cap U$ is uncountable Thus by Limit Point of Subset is Limit Point of Set: :$x$ is limit point of $B$ ...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Let $A, B$ be [[Definition:Subset|subsets]] of $S$. Then: :$A \subseteq B \implies {A^0} \subseteq B^0$ where :$A^0$ denotes the [[Definition:Set of Condensation Points|set of condensation points]] of $A$
Assume :$A \subseteq B$ Let $x \in A^0$. By definition of [[Definition:Set of Condensation Points|set of condensation points]]: :$x$ is [[Definition:Condensation Point|condensation point]] of $A$ By definition of [[Definition:Condensation Point|condensation point]]: :$x$ is [[Definition:Limit Point of Set|limit poin...
Set of Condensation Points is Monotone
https://proofwiki.org/wiki/Set_of_Condensation_Points_is_Monotone
https://proofwiki.org/wiki/Set_of_Condensation_Points_is_Monotone
[ "Condensation Points" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Set of Condensation Points" ]
[ "Definition:Set of Condensation Points", "Definition:Condensation Point", "Definition:Condensation Point", "Definition:Limit Point/Topology/Set", "Definition:Countable Set", "Limit Point of Subset is Limit Point of Set", "Definition:Limit Point/Topology/Set", "Definition:Condensation Point", "Defini...
proofwiki-10953
First Order ODE/x^2 y' = 3 (x^2 + y^2) arctan (y over x) + x y
is a homogeneous differential equation with solution: :$y = x \tan C x^3$
Let: :$\map M {x, y} = 3 \paren {x^2 + y^2} \arctan \dfrac y x + x y$ :$\map N {x, y} = x^2$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = 3 \paren {\paren {t x}^2 + \paren {t y}^2} \arctan \dfrac {t y} {t x} + t x t y | c = }} {{eqn | r = t^2 \paren {3 \paren {x^2 + y^2} \ar...
is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$y = x \tan C x^3$
Let: :$\map M {x, y} = 3 \paren {x^2 + y^2} \arctan \dfrac y x + x y$ :$\map N {x, y} = x^2$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = 3 \paren {\paren {t x}^2 + \paren {t y}^2} \arctan \dfrac {t y} {t x} + t x t y | c = }} {{eqn | r = t^2 \paren {3 \paren {x^2 + y^2} ...
First Order ODE/x^2 y' = 3 (x^2 + y^2) arctan (y over x) + x y
https://proofwiki.org/wiki/First_Order_ODE/x^2_y'_=_3_(x^2_+_y^2)_arctan_(y_over_x)_+_x_y
https://proofwiki.org/wiki/First_Order_ODE/x^2_y'_=_3_(x^2_+_y^2)_arctan_(y_over_x)_+_x_y
[ "Examples of Homogeneous Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Homogeneous Differential Equation", "Solution to Homogeneous Differential Equation", "Derivative of Arctangent Function", "Primitive of Reciprocal" ]
proofwiki-10954
First Order ODE/x sine (y over x) y' = y sine (y over x) + x
is a homogeneous differential equation with solution: :$\cos \dfrac y x + \ln C x = 0$
Let: :$\map M {x, y} = y \sin \dfrac y x + x$ :$\map N {x, y} = x \sin \dfrac y x$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = t y \sin \dfrac t y t x + t x | c = }} {{eqn | r = t \paren {y \sin \dfrac y x + x} | c = }} {{eqn | r = t \, \map M {x, y} | c = }} ...
is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$\cos \dfrac y x + \ln C x = 0$
Let: :$\map M {x, y} = y \sin \dfrac y x + x$ :$\map N {x, y} = x \sin \dfrac y x$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = t y \sin \dfrac t y t x + t x | c = }} {{eqn | r = t \paren {y \sin \dfrac y x + x} | c = }} {{eqn | r = t \, \map M {x, y} | c = ...
First Order ODE/x sine (y over x) y' = y sine (y over x) + x
https://proofwiki.org/wiki/First_Order_ODE/x_sine_(y_over_x)_y'_=_y_sine_(y_over_x)_+_x
https://proofwiki.org/wiki/First_Order_ODE/x_sine_(y_over_x)_y'_=_y_sine_(y_over_x)_+_x
[ "Examples of Homogeneous Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Homogeneous Differential Equation", "Solution to Homogeneous Differential Equation", "Primitive of Sine Function" ]
proofwiki-10955
First Order ODE/x y' = y + 2 x exp (- y over x)
is a homogeneous differential equation with solution: :$e^{y / x} = \ln x^2 + C$
Let: :$\map M {x, y} = y + 2 x e^{-y/x}$ :$\map N {x, y} = x$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = t y + 2 t x e^{-t y / t x} | c = }} {{eqn | r = t \paren {y + 2 x e^{-y / x} } | c = }} {{eqn | r = t \, \map M {x, y} | c = }} {{end-eqn}} {{begin-eqn}} ...
is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$e^{y / x} = \ln x^2 + C$
Let: :$\map M {x, y} = y + 2 x e^{-y/x}$ :$\map N {x, y} = x$ Put $t x, t y$ for $x, y$: {{begin-eqn}} {{eqn | l = \map M {t x, t y} | r = t y + 2 t x e^{-t y / t x} | c = }} {{eqn | r = t \paren {y + 2 x e^{-y / x} } | c = }} {{eqn | r = t \, \map M {x, y} | c = }} {{end-eqn}} {{begin-eq...
First Order ODE/x y' = y + 2 x exp (- y over x)
https://proofwiki.org/wiki/First_Order_ODE/x_y'_=_y_+_2_x_exp_(-_y_over_x)
https://proofwiki.org/wiki/First_Order_ODE/x_y'_=_y_+_2_x_exp_(-_y_over_x)
[ "Examples of Homogeneous Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Homogeneous Differential Equation", "Solution to Homogeneous Differential Equation", "Primitive of Exponential Function" ]
proofwiki-10956
First Order ODE in form y' = f (a x + b y + c)
The first order ODE: :$\dfrac {\d y} {\d x} = \map f {a x + b y + c}$ can be solved by substituting: :$z := a x + b y + c$ to obtain: :$\ds x = \int \frac {\d z} {b \map f z + a}$
We have: :$\dfrac {\d y} {\d x} = \map f {a x + b y + c}$ Put: : $z := a x + b y + c$ Then: {{begin-eqn}} {{eqn | l = z | r = a x + b y + c | c = }} {{eqn | ll= \leadsto | l = \frac {\d z} {\d x} | r = a + b \dfrac {\d y} {\d x} | c = }} {{eqn | ll= \leadsto | l = \dfrac {\d y} {\d...
The [[Definition:First Order Ordinary Differential Equation|first order ODE]]: :$\dfrac {\d y} {\d x} = \map f {a x + b y + c}$ can be solved by substituting: :$z := a x + b y + c$ to obtain: :$\ds x = \int \frac {\d z} {b \map f z + a}$
We have: :$\dfrac {\d y} {\d x} = \map f {a x + b y + c}$ Put: : $z := a x + b y + c$ Then: {{begin-eqn}} {{eqn | l = z | r = a x + b y + c | c = }} {{eqn | ll= \leadsto | l = \frac {\d z} {\d x} | r = a + b \dfrac {\d y} {\d x} | c = }} {{eqn | ll= \leadsto | l = \dfrac {\d y} {...
First Order ODE in form y' = f (a x + b y + c)
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_f_(a_x_+_b_y_+_c)
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_f_(a_x_+_b_y_+_c)
[ "First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation" ]
[ "Solution to Separable Differential Equation" ]
proofwiki-10957
First Order ODE/y' = (x + y)^2
The first order ODE: :$\dfrac {\d y} {\d x} = \paren {x + y}^2$ has the general solution: :$x + y = \map \tan {x + C}$
Make the substitution: :$z = x + y$ Then from First Order ODE in form $y' = f (a x + b y + c)$ with $a = b = 1$: {{begin-eqn}} {{eqn | l = x | r = \int \frac {\d z} {z^2 + 1} | c = }} {{eqn | r = \arctan z + C_1 | c = Primitive of $\dfrac 1 {x^2 + a^2}$ }} {{eqn | ll= \leadsto | l = y - C_1 ...
The [[Definition:First Order ODE|first order ODE]]: :$\dfrac {\d y} {\d x} = \paren {x + y}^2$ has the [[Definition:General Solution to Differential Equation|general solution]]: :$x + y = \map \tan {x + C}$
Make the substitution: :$z = x + y$ Then from [[First Order ODE in form y' = f (a x + b y + c)|First Order ODE in form $y' = f (a x + b y + c)$]] with $a = b = 1$: {{begin-eqn}} {{eqn | l = x | r = \int \frac {\d z} {z^2 + 1} | c = }} {{eqn | r = \arctan z + C_1 | c = [[Primitive of Reciprocal of x...
First Order ODE/y' = (x + y)^2
https://proofwiki.org/wiki/First_Order_ODE/y'_=_(x_+_y)^2
https://proofwiki.org/wiki/First_Order_ODE/y'_=_(x_+_y)^2
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "First Order ODE in form y' = f (a x + b y + c)", "Primitive of Reciprocal of x squared plus a squared/Arctangent Form" ]
proofwiki-10958
First Order ODE/y' = sin^2 (x - y + 1)
The first order ODE: :$\dfrac {\d y} {\d x} = \map {\sin^2} {x - y + 1}^2$ has the general solution: :$\map \tan {x - y + 1} = x + C$
Make the substitution: :$z = x - y + 1$ Then from First Order ODE in form $y' = f (a x + b y + c)$ with $a = 1, b = - 1$: {{begin-eqn}} {{eqn | l = x | r = \int \frac {\d z} {- \sin^2 z + 1} | c = }} {{eqn | r = \int \frac {\d z} {\cos^2 z} | c = Sum of Squares of Sine and Cosine }} {{eqn | r = \int ...
The [[Definition:First Order ODE|first order ODE]]: :$\dfrac {\d y} {\d x} = \map {\sin^2} {x - y + 1}^2$ has the [[Definition:General Solution to Differential Equation|general solution]]: :$\map \tan {x - y + 1} = x + C$
Make the substitution: :$z = x - y + 1$ Then from [[First Order ODE in form y' = f (a x + b y + c)|First Order ODE in form $y' = f (a x + b y + c)$]] with $a = 1, b = - 1$: {{begin-eqn}} {{eqn | l = x | r = \int \frac {\d z} {- \sin^2 z + 1} | c = }} {{eqn | r = \int \frac {\d z} {\cos^2 z} | c = [...
First Order ODE/y' = sin^2 (x - y + 1)
https://proofwiki.org/wiki/First_Order_ODE/y'_=_sin^2_(x_-_y_+_1)
https://proofwiki.org/wiki/First_Order_ODE/y'_=_sin^2_(x_-_y_+_1)
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "First Order ODE in form y' = f (a x + b y + c)", "Sum of Squares of Sine and Cosine", "Secant is Reciprocal of Cosine", "Primitive of Square of Secant Function" ]
proofwiki-10959
First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))
The first order ODE: :$\dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ such that: :$ a e \ne b d$ can be solved by substituting: :$x := z - h$ :$y := w - k$ where: :$h = \dfrac {c e - b f} {a e - b d}$ :$k = \dfrac {a f - c d} {a e - b d}$ to obtain: :$\dfrac {\d w} {\d z} = \map F {\dfrac {a z...
We have: :$\dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ Make the substitutions: :$x := z - h$ :$y := w - k$ We have: :$\dfrac {\d x} {\d z} = 1$ :$\dfrac {\d y} {\d w} = 1$ Thus: {{begin-eqn}} {{eqn | l = \frac {\d w} {\d z} | r = \map F {\frac {a \paren {z - h} + b \paren {w - k} + c}...
The [[Definition:First Order Ordinary Differential Equation|first order ODE]]: :$\dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ such that: :$ a e \ne b d$ can be solved by substituting: :$x := z - h$ :$y := w - k$ where: :$h = \dfrac {c e - b f} {a e - b d}$ :$k = \dfrac {a f - c d} {a e - ...
We have: :$\dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ Make the substitutions: :$x := z - h$ :$y := w - k$ We have: :$\dfrac {\d x} {\d z} = 1$ :$\dfrac {\d y} {\d w} = 1$ Thus: {{begin-eqn}} {{eqn | l = \frac {\d w} {\d z} | r = \map F {\frac {a \paren {z - h} + b \paren {w - k} ...
First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_F_((a_x_+_b_y_+_c)_over_(d_x_+_e_y_+_f))
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_F_((a_x_+_b_y_+_c)_over_(d_x_+_e_y_+_f))
[ "First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))", "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Solution to Homogeneous Differential Equation" ]
[ "Definition:Homogeneous Differential Equation" ]
proofwiki-10960
First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f)) where a e = b d/Formulation 1
The first order ODE: :$(1): \quad \dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ such that: :$a e = b d$ can be solved by substituting: :$z = a x + b y$ to obtain: :$\dfrac {\d z} {\d x} = b \map F {\dfrac {a z + a c} {d z + a f} } + a$ which can be solved by Solution to Separable Differential...
When $a e = b d$, it is not possible to make the substitutions: :$x := z - h$ :$y := w - k$ where: :$h = \dfrac {c e - b f} {a e - b d}$ :$k = \dfrac {a f - c d} {a e - b d}$ and so to use the technique of First Order ODE in form $y' = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$. So, we consider what needs to be ...
The [[Definition:First Order Ordinary Differential Equation|first order ODE]]: :$(1): \quad \dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ such that: :$a e = b d$ can be solved by substituting: :$z = a x + b y$ to obtain: :$\dfrac {\d z} {\d x} = b \map F {\dfrac {a z + a c} {d z + a f} }...
When $a e = b d$, it is not possible to make the substitutions: :$x := z - h$ :$y := w - k$ where: :$h = \dfrac {c e - b f} {a e - b d}$ :$k = \dfrac {a f - c d} {a e - b d}$ and so to use the technique of [[First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))|First Order ODE in form $y' = \map F {\...
First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f)) where a e = b d/Formulation 1
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_F_((a_x_+_b_y_+_c)_over_(d_x_+_e_y_+_f))_where_a_e_=_b_d/Formulation_1
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_F_((a_x_+_b_y_+_c)_over_(d_x_+_e_y_+_f))_where_a_e_=_b_d/Formulation_1
[ "First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))" ]
[ "Definition:First Order Ordinary Differential Equation", "Solution to Separable Differential Equation" ]
[ "First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))", "Definition:Separable Differential Equation", "Definition:Separable Differential Equation", "Definition:Separable Differential Equation" ]
proofwiki-10961
First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f)) where a e = b d/Formulation 2
The first order ODE: :$(1): \quad \dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ such that: :$a e = b d$ can be solved by substituting: :$z = d x + e y$ to obtain: :$\dfrac {\d z} {\d x} = e \map F {\dfrac {b z + e c} {e z + e f} } + d$ which can be solved by Solution to Separable Differential...
When $a e = b d$, it is not possible to make the substitutions: :$x := z - h$ :$y := w - k$ where: :$h = \dfrac {c e - b f} {a e - b d}$ :$k = \dfrac {a f - c d} {a e - b d}$ and so to use the technique of First Order ODE in form $y' = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$. So, we consider what needs to be ...
The [[Definition:First Order Ordinary Differential Equation|first order ODE]]: :$(1): \quad \dfrac {\d y} {\d x} = \map F {\dfrac {a x + b y + c} {d x + e y + f} }$ such that: :$a e = b d$ can be solved by substituting: :$z = d x + e y$ to obtain: :$\dfrac {\d z} {\d x} = e \map F {\dfrac {b z + e c} {e z + e f} }...
When $a e = b d$, it is not possible to make the substitutions: :$x := z - h$ :$y := w - k$ where: :$h = \dfrac {c e - b f} {a e - b d}$ :$k = \dfrac {a f - c d} {a e - b d}$ and so to use the technique of [[First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))|First Order ODE in form $y' = \map F {\...
First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f)) where a e = b d/Formulation 2
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_F_((a_x_+_b_y_+_c)_over_(d_x_+_e_y_+_f))_where_a_e_=_b_d/Formulation_2
https://proofwiki.org/wiki/First_Order_ODE_in_form_y'_=_F_((a_x_+_b_y_+_c)_over_(d_x_+_e_y_+_f))_where_a_e_=_b_d/Formulation_2
[ "First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))" ]
[ "Definition:First Order Ordinary Differential Equation", "Solution to Separable Differential Equation" ]
[ "First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))", "Definition:Separable Differential Equation", "Definition:Separable Differential Equation", "Definition:Separable Differential Equation", "Category:First Order ODE in form y' = F ((a x + b y + c) over (d x + e y + f))" ]
proofwiki-10962
First Order ODE/exp y dx + (x exp y + 2 y) dy = 0
is an exact differential equation with solution: :$x e^y + y^2 = C$
Let: :$\map M {x, y} = e^y$ :$\map N {x, y} = x e^y + 2 y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = e^y | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = e^y | c = }} {{end-eqn}} Thus $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$ ...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$x e^y + y^2 = C$
Let: :$\map M {x, y} = e^y$ :$\map N {x, y} = x e^y + 2 y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = e^y | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = e^y | c = }} {{end-eqn}} Thus $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x...
First Order ODE/exp y dx + (x exp y + 2 y) dy = 0
https://proofwiki.org/wiki/First_Order_ODE/exp_y_dx_+_(x_exp_y_+_2_y)_dy_=_0
https://proofwiki.org/wiki/First_Order_ODE/exp_y_dx_+_(x_exp_y_+_2_y)_dy_=_0
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10963
First Order ODE/(x + (2 over y)) dy + y dx = 0
is an exact differential equation with solution: :$x y + 2 \ln y = C$
Let: :$\map M {x, y} = y$ :$\map N {x, y} = x + \dfrac 2 y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = 1 | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = 1 | c = }} {{end-eqn}} Thus $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$ and...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$x y + 2 \ln y = C$
Let: :$\map M {x, y} = y$ :$\map N {x, y} = x + \dfrac 2 y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = 1 | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = 1 | c = }} {{end-eqn}} Thus $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$ ...
First Order ODE/(x + (2 over y)) dy + y dx = 0
https://proofwiki.org/wiki/First_Order_ODE/(x_+_(2_over_y))_dy_+_y_dx_=_0
https://proofwiki.org/wiki/First_Order_ODE/(x_+_(2_over_y))_dy_+_y_dx_=_0
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10964
First Order ODE/(y - x^3) dx + (x + y^3) dy = 0
is an exact differential equation with solution: :$4 x y - x^4 + y^4 = C$
Let: :$\map M {x, y} = y - x^3$ :$\map N {x, y} = x + y^3$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = 1 | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = 1 | c = }} {{end-eqn}} Thus $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$ and ...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$4 x y - x^4 + y^4 = C$
Let: :$\map M {x, y} = y - x^3$ :$\map N {x, y} = x + y^3$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = 1 | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = 1 | c = }} {{end-eqn}} Thus $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$ a...
First Order ODE/(y - x^3) dx + (x + y^3) dy = 0
https://proofwiki.org/wiki/First_Order_ODE/(y_-_x^3)_dx_+_(x_+_y^3)_dy_=_0
https://proofwiki.org/wiki/First_Order_ODE/(y_-_x^3)_dx_+_(x_+_y^3)_dy_=_0
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10965
First Order ODE/(y + y cosine x y) dx + (x + x cosine x y) dy = 0
is an exact differential equation with solution: :$x y + \sin x y = C$
Let: :$\map M {x, y} = y + y \cos x y$ :$\map N {x, y} = x + x \cos x y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = 1 + \cos x y - x \sin x y | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = 1 + \cos x y - x \sin x y | c = }} {{end-eqn}} Thus $\dfrac {\...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$x y + \sin x y = C$
Let: :$\map M {x, y} = y + y \cos x y$ :$\map N {x, y} = x + x \cos x y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = 1 + \cos x y - x \sin x y | c = }} {{eqn | l = \dfrac {\partial N} {\partial x} | r = 1 + \cos x y - x \sin x y | c = }} {{end-eqn}} Thus $\dfrac...
First Order ODE/(y + y cosine x y) dx + (x + x cosine x y) dy = 0
https://proofwiki.org/wiki/First_Order_ODE/(y_+_y_cosine_x_y)_dx_+_(x_+_x_cosine_x_y)_dy_=_0
https://proofwiki.org/wiki/First_Order_ODE/(y_+_y_cosine_x_y)_dx_+_(x_+_x_cosine_x_y)_dy_=_0
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10966
First Order ODE/(sine x sine y - x e^y) dy = (e^y + cosine x cosine y) dx
is an exact differential equation with solution: :$\sin x \cos y + x e^y = C$
First express $(1)$ in the form: :$(2): \quad -\paren {e^y + \cos x \cos y} + \paren {\sin x \sin y - x e^y} \dfrac {\d y} {\d x}$ Let: :$\map M {x, y} = -\paren {e^y + \cos x \cos y}$ :$\map N {x, y} = \sin x \sin y - x e^y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = -e^y + \cos x \si...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$\sin x \cos y + x e^y = C$
First express $(1)$ in the form: :$(2): \quad -\paren {e^y + \cos x \cos y} + \paren {\sin x \sin y - x e^y} \dfrac {\d y} {\d x}$ Let: :$\map M {x, y} = -\paren {e^y + \cos x \cos y}$ :$\map N {x, y} = \sin x \sin y - x e^y$ Then: {{begin-eqn}} {{eqn | l = \dfrac {\partial M} {\partial y} | r = -e^y + \cos x \...
First Order ODE/(sine x sine y - x e^y) dy = (e^y + cosine x cosine y) dx
https://proofwiki.org/wiki/First_Order_ODE/(sine_x_sine_y_-_x_e^y)_dy_=_(e^y_+_cosine_x_cosine_y)_dx
https://proofwiki.org/wiki/First_Order_ODE/(sine_x_sine_y_-_x_e^y)_dy_=_(e^y_+_cosine_x_cosine_y)_dx
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10967
First Order ODE/-1 over y sine x over y dx + x over y^2 sine x over y dy
is an exact differential equation with solution: :$\dfrac x y = C$
Let: :$\map M {x, y} = -\dfrac 1 y \sin \dfrac x y$ :$\map N {x, y} = \dfrac x {y^2} \sin \dfrac x y$ Then: {{begin-eqn}} {{eqn | l = \frac {\partial M} {\partial y} | r = \frac 1 {y^2} \sin \frac x y + \paren {-\frac 1 y} \paren {-\frac 1 {y^2} } x \cos \frac x y | c = }} {{eqn | r = \frac 1 {y^2} \sin \f...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$\dfrac x y = C$
Let: :$\map M {x, y} = -\dfrac 1 y \sin \dfrac x y$ :$\map N {x, y} = \dfrac x {y^2} \sin \dfrac x y$ Then: {{begin-eqn}} {{eqn | l = \frac {\partial M} {\partial y} | r = \frac 1 {y^2} \sin \frac x y + \paren {-\frac 1 y} \paren {-\frac 1 {y^2} } x \cos \frac x y | c = }} {{eqn | r = \frac 1 {y^2} \sin \...
First Order ODE/-1 over y sine x over y dx + x over y^2 sine x over y dy
https://proofwiki.org/wiki/First_Order_ODE/-1_over_y_sine_x_over_y_dx_+_x_over_y^2_sine_x_over_y_dy
https://proofwiki.org/wiki/First_Order_ODE/-1_over_y_sine_x_over_y_dx_+_x_over_y^2_sine_x_over_y_dy
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Integration by Substitution", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10968
First Order ODE/(2 x y^3 + y cosine x) dx + (3 x^2 y^2 + sine x) dy
is an exact differential equation with solution: :$x^2 y^3 + y \sin x = C$
Let: :$\map M {x, y} = 2 x y^3 + y \cos x$ :$\map N {x, y} = 3 x^2 y^2 + \sin x$ Then: {{begin-eqn}} {{eqn | l = \frac {\partial M} {\partial y} | r = 2 x \cdot 3 y^2 + \cos x | c = }} {{eqn | r = 6 x y^2 + \cos x | c = }} {{eqn | l = \frac {\partial N} {\partial x} | r = 3 x^2 \cdot 2 y^2 + \...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$x^2 y^3 + y \sin x = C$
Let: :$\map M {x, y} = 2 x y^3 + y \cos x$ :$\map N {x, y} = 3 x^2 y^2 + \sin x$ Then: {{begin-eqn}} {{eqn | l = \frac {\partial M} {\partial y} | r = 2 x \cdot 3 y^2 + \cos x | c = }} {{eqn | r = 6 x y^2 + \cos x | c = }} {{eqn | l = \frac {\partial N} {\partial x} | r = 3 x^2 \cdot 2 y^2 + ...
First Order ODE/(2 x y^3 + y cosine x) dx + (3 x^2 y^2 + sine x) dy
https://proofwiki.org/wiki/First_Order_ODE/(2_x_y^3_+_y_cosine_x)_dx_+_(3_x^2_y^2_+_sine_x)_dy
https://proofwiki.org/wiki/First_Order_ODE/(2_x_y^3_+_y_cosine_x)_dx_+_(3_x^2_y^2_+_sine_x)_dy
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10969
First Order ODE/dx = (y over (1 - x^2 y^2)) dx + (x over (1 - x^2 y^2)) dy
is an exact differential equation with solution: :$\map \ln {\dfrac {1 + x y} {1 - x y} } - 2 x = C$
First express $(1)$ in the form: :$(2): \quad \paren {\dfrac y {1 - x^2 y^2} - 1} + \paren {\dfrac x {1 - x^2 y^2} } \dfrac {\d y} {\d x}$ Let: :$\map M {x, y} = \dfrac y {1 - x^2 y^2} - 1$ :$\map N {x, y} = \dfrac x {1 - x^2 y^2}$ Then: {{begin-eqn}} {{eqn | l = \frac {\partial M} {\partial y} | r = \frac {\pare...
is an [[Definition:Exact Differential Equation|exact differential equation]] with [[Definition:General Solution to Differential Equation|solution]]: :$\map \ln {\dfrac {1 + x y} {1 - x y} } - 2 x = C$
First express $(1)$ in the form: :$(2): \quad \paren {\dfrac y {1 - x^2 y^2} - 1} + \paren {\dfrac x {1 - x^2 y^2} } \dfrac {\d y} {\d x}$ Let: :$\map M {x, y} = \dfrac y {1 - x^2 y^2} - 1$ :$\map N {x, y} = \dfrac x {1 - x^2 y^2}$ Then: {{begin-eqn}} {{eqn | l = \frac {\partial M} {\partial y} | r = \frac {\p...
First Order ODE/dx = (y over (1 - x^2 y^2)) dx + (x over (1 - x^2 y^2)) dy
https://proofwiki.org/wiki/First_Order_ODE/dx_=_(y_over_(1_-_x^2_y^2))_dx_+_(x_over_(1_-_x^2_y^2))_dy
https://proofwiki.org/wiki/First_Order_ODE/dx_=_(y_over_(1_-_x^2_y^2))_dx_+_(x_over_(1_-_x^2_y^2))_dy
[ "Examples of Exact Differential Equation", "Examples of First Order ODEs" ]
[ "Definition:Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Quotient Rule for Derivatives", "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Definition:Differential Equation/Solution/General Solution", "Integral Operator is Linear", "Integration by Partial Fractions", "Integral Operator is Linear", "Difference of Logarithm...
proofwiki-10970
Limit Point of Subset is Limit Point of Set
Let $T = \struct {S, \tau}$ be a topological space. Let $A, B$ be subset of $S$ such that :$A \subseteq B$ Let $x$ be a point of $S$. Then: :if $x$ is limit point of $A$, then $x$ is limit point of $B$.
Assume $x$ is limit point of $A$. By definition of limit point it suffices to prove :$\forall U \in \tau: x \in U \implies B \cap \paren {U \setminus \set x} \ne \O$ Let $U \in \tau$ such that :$x \in U$ By definition of limit point: :$A \cap \paren {U \setminus \set x} \ne \O$ By Set Intersection Preserves Subsets/Cor...
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Let $A, B$ be [[Definition:Subset|subset]] of $S$ such that :$A \subseteq B$ Let $x$ be a [[Definition:Element|point]] of $S$. Then: :if $x$ is [[Definition:Limit Point of Set|limit point]] of $A$, then $x$ is [[Definition:Limit Po...
Assume $x$ is [[Definition:Limit Point of Set|limit point]] of $A$. By definition of [[Definition:Limit Point of Set|limit point]] it suffices to prove :$\forall U \in \tau: x \in U \implies B \cap \paren {U \setminus \set x} \ne \O$ Let $U \in \tau$ such that :$x \in U$ By definition of [[Definition:Limit Point of ...
Limit Point of Subset is Limit Point of Set
https://proofwiki.org/wiki/Limit_Point_of_Subset_is_Limit_Point_of_Set
https://proofwiki.org/wiki/Limit_Point_of_Subset_is_Limit_Point_of_Set
[ "Limit Points" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Element", "Definition:Limit Point/Topology/Set", "Definition:Limit Point/Topology/Set" ]
[ "Definition:Limit Point/Topology/Set", "Definition:Limit Point/Topology/Set", "Definition:Limit Point/Topology/Set", "Set Intersection Preserves Subsets/Corollary", "Category:Limit Points" ]
proofwiki-10971
Existence of Infinitely Many Integrating Factors
Let the first order ordinary differential equation: :$(1): \quad \map M {x, y} + \map N {x, y} \dfrac {\d y} {\d x} = 0$ be such that $M$ and $N$ are real functions of two variables which are ''not'' homogeneous functions of the same degree. Suppose $(1)$ has an integrating factor. Then $(1)$ has an infinite number of ...
Let $\map F f$ be any function of $f$ which is an integrating factor of $(1)$. Then: :$\ds \mu \map F f \paren {\map M {x, y} \rd x + \map N {x, y} \rd y} = \map F f \rd f = \map \d {\int \map F f \rd f}$ so $\mu \map F f$ is also an integrating factor. {{qed}}
Let the [[Definition:First Order Ordinary Differential Equation|first order ordinary differential equation]]: :$(1): \quad \map M {x, y} + \map N {x, y} \dfrac {\d y} {\d x} = 0$ be such that $M$ and $N$ are [[Definition:Real Function|real functions]] of two variables which are ''not'' [[Definition:Homogeneous Real Fun...
Let $\map F f$ be any function of $f$ which is an [[Definition:Integrating Factor|integrating factor]] of $(1)$. Then: :$\ds \mu \map F f \paren {\map M {x, y} \rd x + \map N {x, y} \rd y} = \map F f \rd f = \map \d {\int \map F f \rd f}$ so $\mu \map F f$ is also an [[Definition:Integrating Factor|integrating factor]...
Existence of Infinitely Many Integrating Factors
https://proofwiki.org/wiki/Existence_of_Infinitely_Many_Integrating_Factors
https://proofwiki.org/wiki/Existence_of_Infinitely_Many_Integrating_Factors
[ "Integrating Factors" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Real Function", "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Integrating Factor", "Definition:Infinite", "Definition:Integrating Factor" ]
[ "Definition:Integrating Factor", "Definition:Integrating Factor" ]
proofwiki-10972
Integrating Factor for First Order ODE/Preliminary Work
Let the first order ordinary differential equation: :$(1): \quad \map M {x, y} + \map N {x, y} \dfrac {\d y} {\d x} = 0$ be non-homogeneous and not exact. Let $\map \mu x$ be an integrating factor for $(1)$. Let: :$\map P {x, y} := \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Then: :$\dfrac 1 \m...
Let us for ease of manipulation express $(1)$ in the form of differentials: :$(2): \quad \map M {x, y} \rd x + \map N {x, y} \rd y = 0$ Let $\mu$ be an integrating factor for $(2)$. Then, by definition: :$\mu \, \map M {x, y} \rd x + \mu \, \map N {x, y} \rd y = 0$ is an exact differential equation. By Solution to Exac...
Let the [[Definition:First Order Ordinary Differential Equation|first order ordinary differential equation]]: :$(1): \quad \map M {x, y} + \map N {x, y} \dfrac {\d y} {\d x} = 0$ be non-[[Definition:Homogeneous Differential Equation|homogeneous]] and not [[Definition:Exact Differential Equation|exact]]. Let $\map \mu ...
Let us for ease of manipulation express $(1)$ in the form of [[Definition:Differential of Real Function|differentials]]: :$(2): \quad \map M {x, y} \rd x + \map N {x, y} \rd y = 0$ Let $\mu$ be an [[Definition:Integrating Factor|integrating factor]] for $(2)$. Then, by definition: :$\mu \, \map M {x, y} \rd x + \mu \...
Integrating Factor for First Order ODE/Preliminary Work
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Preliminary_Work
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Preliminary_Work
[ "Integrating Factors" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Homogeneous Differential Equation", "Definition:Exact Differential Equation", "Definition:Integrating Factor" ]
[ "Definition:Differential of Mapping/Real Function", "Definition:Integrating Factor", "Definition:Exact Differential Equation", "Solution to Exact Differential Equation", "Product Rule for Derivatives" ]
proofwiki-10973
Integrating Factor for First Order ODE/Function of One Variable
Suppose that: :$\map g x = \dfrac {\dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x} } {\map N {x, y} }$ is a function of $x$ only. Then: :$\map \mu x = e^{\int \map g x \rd x}$ is an integrating factor for $(1)$. Similarly, suppose that: :$\map h y = \dfrac {\dfrac {\partial M} {\partial y} - \dfrac ...
=== Preliminary Work === {{:Integrating Factor for First Order ODE/Preliminary Work}}
Suppose that: :$\map g x = \dfrac {\dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x} } {\map N {x, y} }$ is a [[Definition:Real Function|function]] of $x$ only. Then: :$\map \mu x = e^{\int \map g x \rd x}$ is an [[Definition:Integrating Factor|integrating factor]] for $(1)$. Similarly, suppose tha...
=== [[Integrating Factor for First Order ODE/Preliminary Work|Preliminary Work]] === {{:Integrating Factor for First Order ODE/Preliminary Work}}
Integrating Factor for First Order ODE/Function of One Variable
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Function_of_One_Variable
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Function_of_One_Variable
[ "Integrating Factors" ]
[ "Definition:Real Function", "Definition:Integrating Factor", "Definition:Real Function", "Definition:Integrating Factor" ]
[ "Integrating Factor for First Order ODE/Preliminary Work" ]
proofwiki-10974
Integrating Factor for First Order ODE/Function of Sum of Variables
Suppose that: :$\map g z = \dfrac {\dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x} } {\map N {x, y} - \map M {x, y} }$ is a function of $z$, where $z = x + y$. Then: :$\map \mu {x + y} = \map \mu z = e^{\int \map g z \rd z}$ is an integrating factor for $(1)$.
=== Preliminary Work === {{:Integrating Factor for First Order ODE/Preliminary Work}}
Suppose that: :$\map g z = \dfrac {\dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x} } {\map N {x, y} - \map M {x, y} }$ is a [[Definition:Real Function|function]] of $z$, where $z = x + y$. Then: :$\map \mu {x + y} = \map \mu z = e^{\int \map g z \rd z}$ is an [[Definition:Integrating Factor|integra...
=== [[Integrating Factor for First Order ODE/Preliminary Work|Preliminary Work]] === {{:Integrating Factor for First Order ODE/Preliminary Work}}
Integrating Factor for First Order ODE/Function of Sum of Variables
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Function_of_Sum_of_Variables
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Function_of_Sum_of_Variables
[ "Integrating Factors" ]
[ "Definition:Real Function", "Definition:Integrating Factor" ]
[ "Integrating Factor for First Order ODE/Preliminary Work" ]
proofwiki-10975
Integrating Factor for First Order ODE/Function of Product of Variables
:$\map g z = \dfrac {\dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}} {N y - M x}$ is a function of $z$, where $z = x y$. Then: :$\map \mu {x y} = \map \mu z = e^{\int \map g z \d z}$ is an integrating factor for $(1)$.
=== Preliminary Work === {{:Integrating Factor for First Order ODE/Preliminary Work}}
:$\map g z = \dfrac {\dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}} {N y - M x}$ is a [[Definition:Real Function|function]] of $z$, where $z = x y$. Then: :$\map \mu {x y} = \map \mu z = e^{\int \map g z \d z}$ is an [[Definition:Integrating Factor|integrating factor]] for $(1)$.
=== [[Integrating Factor for First Order ODE/Preliminary Work|Preliminary Work]] === {{:Integrating Factor for First Order ODE/Preliminary Work}}
Integrating Factor for First Order ODE/Function of Product of Variables
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Function_of_Product_of_Variables
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Function_of_Product_of_Variables
[ "Integrating Factors" ]
[ "Definition:Real Function", "Definition:Integrating Factor" ]
[ "Integrating Factor for First Order ODE/Preliminary Work" ]
proofwiki-10976
Set of Condensation Points of Union is Union of Sets of Condensation Points
Let $T = \left({S, \tau}\right)$ be a topological space. Let $A, B$ be subsets of $S$. Then: :$\left({A \cup B}\right)^0 = A^0 \cup B^0$
=== Set of Condensation Points of Union Subset Union of Sets of Condensation Points === Let $x \in \left({A \cup B}\right)^0$. By definition of set of condensation points: :$x$ is condensation point of $A \cup B$ By Lemma: :$x$ is condensation point of $A$ or $x$ is condensation point of $B$ By definition of set of con...
Let $T = \left({S, \tau}\right)$ be a [[Definition:Topological Space|topological space]]. Let $A, B$ be [[Definition:Subset|subsets]] of $S$. Then: :$\left({A \cup B}\right)^0 = A^0 \cup B^0$
=== Set of Condensation Points of Union Subset Union of Sets of Condensation Points === Let $x \in \left({A \cup B}\right)^0$. By definition of [[Definition:Set of Condensation Points|set of condensation points]]: :$x$ is [[Definition:Condensation Point|condensation point]] of $A \cup B$ By [[Set of Condensation Poi...
Set of Condensation Points of Union is Union of Sets of Condensation Points
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Union_is_Union_of_Sets_of_Condensation_Points
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Union_is_Union_of_Sets_of_Condensation_Points
[ "Condensation Points" ]
[ "Definition:Topological Space", "Definition:Subset" ]
[ "Definition:Set of Condensation Points", "Definition:Condensation Point", "Set of Condensation Points of Union is Union of Sets of Condensation Points/Lemma", "Definition:Condensation Point", "Definition:Condensation Point", "Definition:Set of Condensation Points", "Definition:Set Union" ]
proofwiki-10977
Set of Condensation Points of Union is Union of Sets of Condensation Points/Lemma
Let $x$ be a point of $S$. Then: :if $x$ is condensation point of $A \cup B$, :then $x$ is condensation point of $A$ or $x$ is condensation point of $B$.
Assume $x$ is condensation point of $A \cup B$. {{AimForCont}} :$x$ is not condensation point of $A$ and $x$ is not condensation point of $B$. By definition of condensation point: :$\exists U_1 \in \tau: x \in U_1 \land A \cap U_1$ is countable By definition of condensation point: :$\exists U_2 \in \tau: x \in U_2 \lan...
Let $x$ be a [[Definition:Element|point]] of $S$. Then: :if $x$ is [[Definition:Condensation Point|condensation point]] of $A \cup B$, :then $x$ is [[Definition:Condensation Point|condensation point]] of $A$ or $x$ is [[Definition:Condensation Point|condensation point]] of $B$.
Assume $x$ is [[Definition:Condensation Point|condensation point]] of $A \cup B$. {{AimForCont}} :$x$ is not [[Definition:Condensation Point|condensation point]] of $A$ and $x$ is not [[Definition:Condensation Point|condensation point]] of $B$. By definition of [[Definition:Condensation Point|condensation point]]: :$...
Set of Condensation Points of Union is Union of Sets of Condensation Points/Lemma
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Union_is_Union_of_Sets_of_Condensation_Points/Lemma
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Union_is_Union_of_Sets_of_Condensation_Points/Lemma
[ "Condensation Points" ]
[ "Definition:Element", "Definition:Condensation Point", "Definition:Condensation Point", "Definition:Condensation Point" ]
[ "Definition:Condensation Point", "Definition:Condensation Point", "Definition:Condensation Point", "Definition:Condensation Point", "Definition:Countable Set", "Definition:Condensation Point", "Definition:Countable Set", "Definition:Set Intersection", "Definition:Topological Space", "Intersection ...
proofwiki-10978
Integrating Factor for First Order ODE/Conclusion
Let the first order ordinary differential equation: :$(1): \quad \map M {x, y} + \map N {x, y} \dfrac {\d y} {\d x} = 0$ be non-homogeneous and not exact. Let $\map \mu {x, y}$be an integrating factor for $(1)$. If one of these is the case: :$\mu$ is a function of $x$ only :$\mu$ is a function of $y$ only :$\mu$ is a f...
We have an equation of the form: :$\dfrac 1 \mu \dfrac {\d \mu} {\d w} = \map f w$ which is what you get when you apply the Chain Rule for Derivatives and Derivative of Logarithm Function to: :$\dfrac {\map \d {\ln \mu} } {\d w} = \map f w$ Thus: :$\ds \ln \mu = \int \map f w \rd w$ and so: :$\mu = e^{\int \map f w \rd...
Let the [[Definition:First Order Ordinary Differential Equation|first order ordinary differential equation]]: :$(1): \quad \map M {x, y} + \map N {x, y} \dfrac {\d y} {\d x} = 0$ be non-[[Definition:Homogeneous Differential Equation|homogeneous]] and not [[Definition:Exact Differential Equation|exact]]. Let $\map \mu ...
We have an equation of the form: :$\dfrac 1 \mu \dfrac {\d \mu} {\d w} = \map f w$ which is what you get when you apply the [[Chain Rule for Derivatives]] and [[Derivative of Logarithm Function]] to: :$\dfrac {\map \d {\ln \mu} } {\d w} = \map f w$ Thus: :$\ds \ln \mu = \int \map f w \rd w$ and so: :$\mu = e^{\int \m...
Integrating Factor for First Order ODE/Conclusion
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Conclusion
https://proofwiki.org/wiki/Integrating_Factor_for_First_Order_ODE/Conclusion
[ "Integrating Factors" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Homogeneous Differential Equation", "Definition:Exact Differential Equation", "Definition:Integrating Factor" ]
[ "Derivative of Composite Function", "Derivative of Logarithm Function" ]
proofwiki-10979
First Order ODE/y dx + (x^2 y - x) dy = 0
The first order ODE: :$(1): \quad y \rd x + \paren {x^2 y - x} \rd y = 0$ has the general solution: :$\dfrac {y^2} 2 - \dfrac y x = C$
We note that $(1)$ is in the form: :$\map M {x, y} \d x + \map N {x, y} \d y = 0$ but that $(1)$ is not exact. So, let: :$\map M {x, y} = y$ :$\map N {x, y} = x^2 y - x$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Thus: {{begin-eqn}} {{eqn | l = \map P {x, y} | r = ...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad y \rd x + \paren {x^2 y - x} \rd y = 0$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$\dfrac {y^2} 2 - \dfrac y x = C$
We note that $(1)$ is in the form: :$\map M {x, y} \d x + \map N {x, y} \d y = 0$ but that $(1)$ is not [[Definition:Exact Differential Equation|exact]]. So, let: :$\map M {x, y} = y$ :$\map N {x, y} = x^2 y - x$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Thus: {{beg...
First Order ODE/y dx + (x^2 y - x) dy = 0/Proof 1
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_(x^2_y_-_x)_dy_=_0
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_(x^2_y_-_x)_dy_=_0/Proof_1
[ "Examples of First Order ODEs", "First Order ODE/y dx + (x^2 y - x) dy = 0" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Integrating Factor for First Order ODE/Function of One Variable", "Definition:Integrating Factor", "Definition:Exact Differential Equation", "First Order ODE/(y over x^2) dx + (y - 1 over x) dy = 0" ]
proofwiki-10980
First Order ODE/y dx + (x^2 y - x) dy = 0
The first order ODE: :$(1): \quad y \rd x + \paren {x^2 y - x} \rd y = 0$ has the general solution: :$\dfrac {y^2} 2 - \dfrac y x = C$
Rearranging, we have: :$x^2 y \rd y - \paren {x \rd y - y \rd x} = 0$ Aiming to use Quotient Rule for Differentials, divide by $x^2$: :$y \rd y = \dfrac {x \rd y - y \rd x} {x^2}$ So from Quotient Rule for Differentials: Formulation 1 :$y \rd y = \map \d {\dfrac y x}$ from which the solution immediately drops: :$\dfrac...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad y \rd x + \paren {x^2 y - x} \rd y = 0$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$\dfrac {y^2} 2 - \dfrac y x = C$
Rearranging, we have: :$x^2 y \rd y - \paren {x \rd y - y \rd x} = 0$ Aiming to use [[Quotient Rule for Differentials]], divide by $x^2$: :$y \rd y = \dfrac {x \rd y - y \rd x} {x^2}$ So from [[Quotient Rule for Differentials/Formulation 1|Quotient Rule for Differentials: Formulation 1]] :$y \rd y = \map \d {\dfrac y...
First Order ODE/y dx + (x^2 y - x) dy = 0/Proof 2
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_(x^2_y_-_x)_dy_=_0
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_(x^2_y_-_x)_dy_=_0/Proof_2
[ "Examples of First Order ODEs", "First Order ODE/y dx + (x^2 y - x) dy = 0" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Quotient Rule for Differentials", "Quotient Rule for Differentials/Formulation 1" ]
proofwiki-10981
Set of Condensation Points of Countable Set is Empty
Let $T = \struct {S, \tau}$ be a topological space. Let $A$ be a subset of $S$. Then: :if $A$ is countable, :then $A^0 = \O$.
Assume :$A$ is countable. {{AimForCont}} :$A^0 \ne \O$ By definition of empty set: :$\exists x: x \in A^0$ Then by definition of set of condensation points: :$x$ is a condensation point of $A$. This contradicts Lemma. Thus the result follows by Proof by Contradiction. {{qed}}
Let $T = \struct {S, \tau}$ be a [[Definition:Topological Space|topological space]]. Let $A$ be a [[Definition:Subset|subset]] of $S$. Then: :if $A$ is [[Definition:Countable Set|countable]], :then $A^0 = \O$.
Assume :$A$ is [[Definition:Countable Set|countable]]. {{AimForCont}} :$A^0 \ne \O$ By definition of [[Definition:Empty Set|empty set]]: :$\exists x: x \in A^0$ Then by definition of [[Definition:Set of Condensation Points|set of condensation points]]: :$x$ is a [[Definition:Condensation Point|condensation point]] o...
Set of Condensation Points of Countable Set is Empty
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Countable_Set_is_Empty
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Countable_Set_is_Empty
[ "Condensation Points" ]
[ "Definition:Topological Space", "Definition:Subset", "Definition:Countable Set" ]
[ "Definition:Countable Set", "Definition:Empty Set", "Definition:Set of Condensation Points", "Definition:Condensation Point", "Set of Condensation Points of Countable Set is Empty/Lemma", "Proof by Contradiction" ]
proofwiki-10982
Set of Condensation Points of Countable Set is Empty/Lemma
:if $A$ is countable, :then there exists no point $x$ of $S$ such that $x$ is a condensation point of $A$.
Assume :$A$ is countable. {{AimForCont}} there exists a point $x$ of $S$ such that : $x$ is a condensation point of $A$ By definition of topological space: :$S \in \tau$ Then by definition of condensation point: :$A \cap S$ is uncountable By Intersection with Subset is Subset: :$A \cap S = A$ $A$ is countable contradic...
:if $A$ is [[Definition:Countable Set|countable]], :then there exists no [[Definition:Element|point]] $x$ of $S$ such that $x$ is a [[Definition:Condensation Point|condensation point]] of $A$.
Assume :$A$ is [[Definition:Countable Set|countable]]. {{AimForCont}} there exists a [[Definition:Element|point]] $x$ of $S$ such that : $x$ is a [[Definition:Condensation Point|condensation point]] of $A$ By definition of [[Definition:Topological Space|topological space]]: :$S \in \tau$ Then by definition of [[Defi...
Set of Condensation Points of Countable Set is Empty/Lemma
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Countable_Set_is_Empty/Lemma
https://proofwiki.org/wiki/Set_of_Condensation_Points_of_Countable_Set_is_Empty/Lemma
[ "Condensation Points" ]
[ "Definition:Countable Set", "Definition:Element", "Definition:Condensation Point" ]
[ "Definition:Countable Set", "Definition:Element", "Definition:Condensation Point", "Definition:Topological Space", "Definition:Condensation Point", "Definition:Countable Set", "Intersection with Subset is Subset", "Definition:Countable Set", "Definition:Countable Set", "Proof by Contradiction" ]
proofwiki-10983
First Order ODE/(3 x^2 - y^2) dy - 2 x y dx = 0
The first order ODE: :$(1): \quad \paren {3 x^2 - y^2} \rd y - 2 x y \rd x = 0$ has the general solution: :$\dfrac 1 y - \dfrac {x^2} {y^3} = C$
We note that $(1)$ is in the form: :$\map M {x, y} \rd x + \map N {x, y} \rd y = 0$ but that $(1)$ is not exact. So, let: :$\map M {x, y} = -2 x y$ :$\map N {x, y} = 3 x^2 - y^2$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Thus: {{begin-eqn}} {{eqn | l = \map P {x, y} ...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad \paren {3 x^2 - y^2} \rd y - 2 x y \rd x = 0$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$\dfrac 1 y - \dfrac {x^2} {y^3} = C$
We note that $(1)$ is in the form: :$\map M {x, y} \rd x + \map N {x, y} \rd y = 0$ but that $(1)$ is not [[Definition:Exact Differential Equation|exact]]. So, let: :$\map M {x, y} = -2 x y$ :$\map N {x, y} = 3 x^2 - y^2$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Th...
First Order ODE/(3 x^2 - y^2) dy - 2 x y dx = 0
https://proofwiki.org/wiki/First_Order_ODE/(3_x^2_-_y^2)_dy_-_2_x_y_dx_=_0
https://proofwiki.org/wiki/First_Order_ODE/(3_x^2_-_y^2)_dy_-_2_x_y_dx_=_0
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Integrating Factor for First Order ODE/Function of One Variable", "Definition:Integrating Factor", "Definition:Exact Differential Equation", "First Order ODE/(3 x^2 over y^4 - 1 over y^2) dy - 2 x over y^3 dx = 0" ]
proofwiki-10984
First Order ODE/(x y - 1) dx + (x^2 - x y) dy = 0
The first order ODE: :$(1): \quad \paren {x y - 1} \rd x + \paren {x^2 - x y} \rd y = 0$ has the general solution: :$x y - \ln x - \dfrac {y^2} 2 + C$
We note that $(1)$ is in the form: :$\map M {x, y} \rd x + \map N {x, y} \rd y = 0$ but that $(1)$ is not exact. So, let: :$\map M {x, y} = x y - 1$ :$\map N {x, y} = x^2 - x y = x \paren {x - y}$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Thus: {{begin-eqn}} {{eqn | l =...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad \paren {x y - 1} \rd x + \paren {x^2 - x y} \rd y = 0$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$x y - \ln x - \dfrac {y^2} 2 + C$
We note that $(1)$ is in the form: :$\map M {x, y} \rd x + \map N {x, y} \rd y = 0$ but that $(1)$ is not [[Definition:Exact Differential Equation|exact]]. So, let: :$\map M {x, y} = x y - 1$ :$\map N {x, y} = x^2 - x y = x \paren {x - y}$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N}...
First Order ODE/(x y - 1) dx + (x^2 - x y) dy = 0
https://proofwiki.org/wiki/First_Order_ODE/(x_y_-_1)_dx_+_(x^2_-_x_y)_dy_=_0
https://proofwiki.org/wiki/First_Order_ODE/(x_y_-_1)_dx_+_(x^2_-_x_y)_dy_=_0
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Integrating Factor for First Order ODE/Function of One Variable", "Definition:Integrating Factor", "Definition:Exact Differential Equation", "First Order ODE/(y - 1 over x) dx + (x - y) dy = 0" ]
proofwiki-10985
First Order ODE/y dx + x dy + 3 x^3 y^4 dy
The first order ODE: :$(1): \quad y \rd x + x \rd y + 3 x^3 y^4 \rd y = 0$ has the general solution: :$-\dfrac 1 {2 x^2 y^2} + \dfrac {3 y^2} 2 = C$
We note that $(1)$ is in the form: :$\map M {x, y} \rd x + \map N {x, y} \rd y = 0$ but that $(1)$ is not exact. So, let: :$\map M {x, y} = y$ :$\map N {x, y} = 3 x^3 y^4 + x = x \paren {3 x^2 y^4 + 1}$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Thus: {{begin-eqn}} {{eqn...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad y \rd x + x \rd y + 3 x^3 y^4 \rd y = 0$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$-\dfrac 1 {2 x^2 y^2} + \dfrac {3 y^2} 2 = C$
We note that $(1)$ is in the form: :$\map M {x, y} \rd x + \map N {x, y} \rd y = 0$ but that $(1)$ is not [[Definition:Exact Differential Equation|exact]]. So, let: :$\map M {x, y} = y$ :$\map N {x, y} = 3 x^3 y^4 + x = x \paren {3 x^2 y^4 + 1}$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\part...
First Order ODE/y dx + x dy + 3 x^3 y^4 dy
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_x_dy_+_3_x^3_y^4_dy
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_x_dy_+_3_x^3_y^4_dy
[ "First Order ODE/y dx + x dy + 3 x^3 y^4 dy", "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Exact Differential Equation", "Integrating Factor for First Order ODE/Function of Product of Variables", "Definition:Integrating Factor", "Definition:Exact Differential Equation", "First Order ODE/1 over x^3 y^2 dx + (1 over x^2 y^3 + 3 y) dy = 0" ]
proofwiki-10986
Curved Mirror producing Parallel Rays is Paraboloid
Let $M$ be a curved mirror embedded in a real cartesian $3$- space. Let there be a source of light at the origin. Let $M$ reflect the light in a beam parallel to the $x$-axis. Then $M$ is the solid of revolution produced by rotating about the $x$-axis the parabola whose equation is: :$y^2 = 2 c x + c^2$
The mirror will have the shape of a surface of revolution generated by revolving a curve $APB$ in the cartesian plane around the $x$-axis. Let $P = \tuple {x, y}$ be an arbitrary point on $APB$. :500px From the Law of Reflection: :$\alpha = \beta$ From Parallelism implies Equal Corresponding Angles: :$\phi = \beta$ Fro...
Let $M$ be a [[Definition:Curve|curved]] [[Definition:Mirror|mirror]] embedded in a [[Definition:Real Cartesian Space|real cartesian $3$- space]]. Let there be a source of [[Definition:Light (Radiation)|light]] at the [[Definition:Origin|origin]]. Let $M$ reflect the [[Definition:Light (Radiation)|light]] in a beam [...
The [[Definition:Mirror|mirror]] will have the shape of a [[Definition:Surface of Revolution|surface of revolution]] generated by revolving a [[Definition:Curve|curve]] $APB$ in the [[Definition:Cartesian Plane|cartesian plane]] around the [[Definition:X-Axis|$x$-axis]]. Let $P = \tuple {x, y}$ be an arbitrary [[Defin...
Curved Mirror producing Parallel Rays is Paraboloid
https://proofwiki.org/wiki/Curved_Mirror_producing_Parallel_Rays_is_Paraboloid
https://proofwiki.org/wiki/Curved_Mirror_producing_Parallel_Rays_is_Paraboloid
[ "Optics" ]
[ "Definition:Line/Curve", "Definition:Mirror", "Definition:Cartesian Product/Cartesian Space/Real Cartesian Space", "Definition:Light (Radiation)", "Definition:Coordinate System/Origin", "Definition:Light (Radiation)", "Definition:Parallel (Geometry)/Lines", "Definition:Axis/X-Axis", "Definition:Soli...
[ "Definition:Mirror", "Definition:Surface of Revolution", "Definition:Line/Curve", "Definition:Cartesian Plane", "Definition:Axis/X-Axis", "Definition:Point", "File:ParabolicMirror.png", "Law of Reflection", "Parallelism implies Equal Corresponding Angles", "External Angle of Triangle equals Sum of...
proofwiki-10987
First Order ODE/x dy - y dx = (1 + y^2) dy
The first order ODE: :$(1): \quad x \rd y - y \rd x = \paren {1 + y^2} \rd y$ has the general solution: :$\dfrac x y = \dfrac 1 y - y + C$
Rearranging, we have: :$\dfrac {y \rd x - x \rd y} {y^2} = -\paren {\dfrac 1 {y^2} + 1} \rd y$ From the Quotient Rule for Derivatives: :$\map \d {\dfrac x y} = \dfrac {y \rd x - x \rd y} {y^2}$ from which: :$\map \d {\dfrac x y} = -\paren {\dfrac 1 {y^2} + 1} \rd y$ Hence the result: :$\dfrac x y = \dfrac 1 y - y + C$ ...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad x \rd y - y \rd x = \paren {1 + y^2} \rd y$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$\dfrac x y = \dfrac 1 y - y + C$
Rearranging, we have: :$\dfrac {y \rd x - x \rd y} {y^2} = -\paren {\dfrac 1 {y^2} + 1} \rd y$ From the [[Quotient Rule for Derivatives]]: :$\map \d {\dfrac x y} = \dfrac {y \rd x - x \rd y} {y^2}$ from which: :$\map \d {\dfrac x y} = -\paren {\dfrac 1 {y^2} + 1} \rd y$ Hence the result: :$\dfrac x y = \dfrac 1 y - ...
First Order ODE/x dy - y dx = (1 + y^2) dy
https://proofwiki.org/wiki/First_Order_ODE/x_dy_-_y_dx_=_(1_+_y^2)_dy
https://proofwiki.org/wiki/First_Order_ODE/x_dy_-_y_dx_=_(1_+_y^2)_dy
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Quotient Rule for Derivatives" ]
proofwiki-10988
Differential of Sum of Squares
:$\map \d {x^2 + y^2} = 2 \paren {x \map \rd x + y \map \rd y}$
{{begin-eqn}} {{eqn | l = \map \rd {x^2 + y^2; \vec h} | r = 2 x \vec h_1 + 2 y \vec h_2 | c = {{Defof|Differential of Mapping|subdef = Real-Valued Function}} }} {{eqn | r = 2 x \map \rd {x; \vec h} + 2 y \map \rd {y; \vec h} }} {{eqn | r = 2 \paren {x \map \rd {x; \vec h} + y \map \rd {y; \vec h} } }} {{en...
:$\map \d {x^2 + y^2} = 2 \paren {x \map \rd x + y \map \rd y}$
{{begin-eqn}} {{eqn | l = \map \rd {x^2 + y^2; \vec h} | r = 2 x \vec h_1 + 2 y \vec h_2 | c = {{Defof|Differential of Mapping|subdef = Real-Valued Function}} }} {{eqn | r = 2 x \map \rd {x; \vec h} + 2 y \map \rd {y; \vec h} }} {{eqn | r = 2 \paren {x \map \rd {x; \vec h} + y \map \rd {y; \vec h} } }} {{en...
Differential of Sum of Squares
https://proofwiki.org/wiki/Differential_of_Sum_of_Squares
https://proofwiki.org/wiki/Differential_of_Sum_of_Squares
[ "Differentials" ]
[]
[]
proofwiki-10989
First Order ODE/y dx + (x^2 y - x) dy = 0/Proof 1
{{:First Order ODE/y dx + (x^2 y - x) dy = 0}} This can also be presented in the form: :$\dfrac {\d y} {\d x} + \dfrac y {x^2 y - x}$
We note that $(1)$ is in the form: :$\map M {x, y} \d x + \map N {x, y} \d y = 0$ but that $(1)$ is not exact. So, let: :$\map M {x, y} = y$ :$\map N {x, y} = x^2 y - x$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Thus: {{begin-eqn}} {{eqn | l = \map P {x, y} | r = ...
{{:First Order ODE/y dx + (x^2 y - x) dy = 0}} This can also be presented in the form: :$\dfrac {\d y} {\d x} + \dfrac y {x^2 y - x}$
We note that $(1)$ is in the form: :$\map M {x, y} \d x + \map N {x, y} \d y = 0$ but that $(1)$ is not [[Definition:Exact Differential Equation|exact]]. So, let: :$\map M {x, y} = y$ :$\map N {x, y} = x^2 y - x$ Let: :$\map P {x, y} = \dfrac {\partial M} {\partial y} - \dfrac {\partial N} {\partial x}$ Thus: {{beg...
First Order ODE/y dx + (x^2 y - x) dy = 0/Proof 1
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_(x^2_y_-_x)_dy_=_0/Proof_1
https://proofwiki.org/wiki/First_Order_ODE/y_dx_+_(x^2_y_-_x)_dy_=_0/Proof_1
[ "First Order ODE/y dx + (x^2 y - x) dy = 0" ]
[]
[ "Definition:Exact Differential Equation", "Integrating Factor for First Order ODE/Function of One Variable", "Definition:Integrating Factor", "Definition:Exact Differential Equation", "First Order ODE/(y over x^2) dx + (y - 1 over x) dy = 0" ]
proofwiki-10990
First Order ODE/y dx - x dy = x y^3 dy
The first order ODE: :$(1): \quad y \rd x - x \rd y = x y^3 \rd y$ has the general solution: :$\ln \dfrac x y = \dfrac {y^3} 3 + C$
Rearranging, we have: :$\dfrac {y \rd x - x \rd y} {x y} = y^2 \rd y$ From Differential of Logarithm of Quotient: :$\map \d {\ln \dfrac y x} = \dfrac {y \rd x - x \rd y} {x y}$ from which: :$\map \d {\ln \dfrac x y} = y^2 \rd y$ Hence the result: :$\ln \dfrac x y = \dfrac {y^3} 3 + C$ {{qed}}
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad y \rd x - x \rd y = x y^3 \rd y$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$\ln \dfrac x y = \dfrac {y^3} 3 + C$
Rearranging, we have: :$\dfrac {y \rd x - x \rd y} {x y} = y^2 \rd y$ From [[Differential of Logarithm of Quotient]]: :$\map \d {\ln \dfrac y x} = \dfrac {y \rd x - x \rd y} {x y}$ from which: :$\map \d {\ln \dfrac x y} = y^2 \rd y$ Hence the result: :$\ln \dfrac x y = \dfrac {y^3} 3 + C$ {{qed}}
First Order ODE/y dx - x dy = x y^3 dy
https://proofwiki.org/wiki/First_Order_ODE/y_dx_-_x_dy_=_x_y^3_dy
https://proofwiki.org/wiki/First_Order_ODE/y_dx_-_x_dy_=_x_y^3_dy
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Differential of Logarithm of Quotient" ]
proofwiki-10991
First Order ODE/x dy = (x^5 + x^3 y^2 + y) dx
The first order ODE: :$(1): \quad x \rd y = \paren {x^5 + x^3 y^2 + y} \rd x$ has the general solution: :$\arctan \dfrac x y = -\dfrac {x^4} 4 + C$
Rearranging, we have: :$y \rd x - x \rd y = -\paren {x^2 + y^2} x^3 \rd x$ from which: :$\dfrac {y \rd x - x \rd y} {x^2 + y^2} = - x^3 \rd x$ From Differential of Arctangent of Quotient: :$\map \d {\arctan \dfrac x y} = \dfrac {y \rd x - x \rd y} {x^2 + y^2}$ from which $(1)$ evolves into: :$\map \d {\arctan \dfrac x ...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad x \rd y = \paren {x^5 + x^3 y^2 + y} \rd x$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$\arctan \dfrac x y = -\dfrac {x^4} 4 + C$
Rearranging, we have: :$y \rd x - x \rd y = -\paren {x^2 + y^2} x^3 \rd x$ from which: :$\dfrac {y \rd x - x \rd y} {x^2 + y^2} = - x^3 \rd x$ From [[Differential of Arctangent of Quotient]]: :$\map \d {\arctan \dfrac x y} = \dfrac {y \rd x - x \rd y} {x^2 + y^2}$ from which $(1)$ evolves into: :$\map \d {\arctan \d...
First Order ODE/x dy = (x^5 + x^3 y^2 + y) dx
https://proofwiki.org/wiki/First_Order_ODE/x_dy_=_(x^5_+_x^3_y^2_+_y)_dx
https://proofwiki.org/wiki/First_Order_ODE/x_dy_=_(x^5_+_x^3_y^2_+_y)_dx
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Differential of Arctangent of Quotient" ]
proofwiki-10992
First Order ODE/(x + y) dx = (x - y) dy/Proof 1
The first order ordinary differential equation: :$(1): \quad \paren {x + y} \rd x = \paren {x - y} \rd y$ is a homogeneous differential equation with solution: :$\arctan \dfrac y x = \ln \sqrt{x^2 + y^2} + C$
Let: :$\map M {x, y} = x + y$ :$\map N {x, y} = x - y$ We have that: :$\map M {t x, t y} = t x + t y = t \paren {x + y} = t \map M {x, y}$ :$\map N {t x, t y} = t x - t y = t \paren {x - y} = t \map N {x, y}$ Thus both $M$ and $N$ are homogeneous functions of degree $1$. Thus by definition $(1)$ is a homogeneous di...
The [[Definition:First Order Ordinary Differential Equation|first order ordinary differential equation]]: :$(1): \quad \paren {x + y} \rd x = \paren {x - y} \rd y$ is a [[Definition:Homogeneous Differential Equation|homogeneous differential equation]] with [[Definition:General Solution to Differential Equation|solut...
Let: :$\map M {x, y} = x + y$ :$\map N {x, y} = x - y$ We have that: :$\map M {t x, t y} = t x + t y = t \paren {x + y} = t \map M {x, y}$ :$\map N {t x, t y} = t x - t y = t \paren {x - y} = t \map N {x, y}$ Thus both $M$ and $N$ are [[Definition:Homogeneous Real Function|homogeneous functions]] of [[Definition...
First Order ODE/(x + y) dx = (x - y) dy/Proof 1
https://proofwiki.org/wiki/First_Order_ODE/(x_+_y)_dx_=_(x_-_y)_dy/Proof_1
https://proofwiki.org/wiki/First_Order_ODE/(x_+_y)_dx_=_(x_-_y)_dy/Proof_1
[ "Examples of First Order ODEs" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Homogeneous Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Homogeneous Function/Real Space", "Definition:Homogeneous Function/Real Space/Degree", "Definition:Homogeneous Differential Equation", "Definition:Fraction/Numerator", "Definition:Fraction/Denominator", "Solution to Homogeneous Differential Equation", "Primitive of Reciprocal of x squared pl...
proofwiki-10993
First Order ODE/x dy = (y + x^2 + 9 y^2) dx
The first order ODE: :$(1): \quad x \rd y = \paren {y + x^2 + 9 y^2} \rd x$ has the general solution: :$\map \arctan {\dfrac {3 y} x} = 3 x + C$
Divide both sides of $(1)$ by $x^2 \rd x$ to get: :$\dfrac 1 x \dfrac {\d y} {\d x} = \dfrac 1 x \paren {\dfrac y x } + 1 + 9 \paren {\dfrac y x}^2$ Now apply the substitution: :$y = u x$ This implies then that: :$\dfrac {\d y} {\d x} = u + x \dfrac {\d u} {\d x}$ Now substitute everything into $(1)$ to get: {{begin-eq...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad x \rd y = \paren {y + x^2 + 9 y^2} \rd x$ has the [[Definition:General Solution to Differential Equation|general solution]]: :$\map \arctan {\dfrac {3 y} x} = 3 x + C$
Divide both sides of $(1)$ by $x^2 \rd x$ to get: :$\dfrac 1 x \dfrac {\d y} {\d x} = \dfrac 1 x \paren {\dfrac y x } + 1 + 9 \paren {\dfrac y x}^2$ Now apply the substitution: :$y = u x$ This implies then that: :$\dfrac {\d y} {\d x} = u + x \dfrac {\d u} {\d x}$ Now substitute everything into $(1)$ to get: {{begi...
First Order ODE/x dy = (y + x^2 + 9 y^2) dx/Proof 1
https://proofwiki.org/wiki/First_Order_ODE/x_dy_=_(y_+_x^2_+_9_y^2)_dx
https://proofwiki.org/wiki/First_Order_ODE/x_dy_=_(y_+_x^2_+_9_y^2)_dx/Proof_1
[ "Examples of First Order ODEs", "First Order ODE/x dy = (y + x^2 + 9 y^2) dx" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Solution to Separable Differential Equation" ]
proofwiki-10994
First Order ODE/x dy = (y + x^2 + 9 y^2) dx
The first order ODE: :$(1): \quad x \rd y = \paren {y + x^2 + 9 y^2} \rd x$ has the general solution: :$\map \arctan {\dfrac {3 y} x} = 3 x + C$
Let $z = \map \arctan {3y / x}$. Then: :$\dfrac {\partial z} {\partial x} = \dfrac 1 {1 + \paren {3 y / x}^2} \dfrac {-3 y} {x^2} = \dfrac {-3 y} {x^2 + 9 y^2}$ :$\dfrac {\partial z} {\partial y} = \dfrac 1 {1 + \paren {3 y / x}^2} \dfrac 3 x = \dfrac 3 {x^2 + 9 y^2}$ So: :$\d z = \dfrac {3 x \rd y - 3 y \rd x} {x^2 + ...
The [[Definition:First Order ODE|first order ODE]]: :$(1): \quad x \rd y = \paren {y + x^2 + 9 y^2} \rd x$ has the [[Definition:General Solution to Differential Equation|general solution]]: :$\map \arctan {\dfrac {3 y} x} = 3 x + C$
Let $z = \map \arctan {3y / x}$. Then: :$\dfrac {\partial z} {\partial x} = \dfrac 1 {1 + \paren {3 y / x}^2} \dfrac {-3 y} {x^2} = \dfrac {-3 y} {x^2 + 9 y^2}$ :$\dfrac {\partial z} {\partial y} = \dfrac 1 {1 + \paren {3 y / x}^2} \dfrac 3 x = \dfrac 3 {x^2 + 9 y^2}$ So: :$\d z = \dfrac {3 x \rd y - 3 y \rd x} {x^2...
First Order ODE/x dy = (y + x^2 + 9 y^2) dx/Proof 2
https://proofwiki.org/wiki/First_Order_ODE/x_dy_=_(y_+_x^2_+_9_y^2)_dx
https://proofwiki.org/wiki/First_Order_ODE/x_dy_=_(y_+_x^2_+_9_y^2)_dx/Proof_2
[ "Examples of First Order ODEs", "First Order ODE/x dy = (y + x^2 + 9 y^2) dx" ]
[ "Definition:First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Differential of Arctangent of Quotient" ]
proofwiki-10995
Linear First Order ODE/y' + (y over x) = 3 x
The linear first order ODE: :$\dfrac {\d y} {\d x} + \dfrac y x = 3 x$ has the general solution: :$x y = x^3 + C$ or: :$y = x^2 + \dfrac C x$
This is a special case of: :Linear First Order ODE: $\dfrac {\d y} {\d x} + \dfrac y x = k x^n$ where $k = 3$ and $n = 1$, yielding: :$y = x^2 + \dfrac C x$ Multiplying through by $x$ reveals: :$x y = x^3 + C$ {{qed}}
The [[Definition:Linear First Order ODE|linear first order ODE]]: :$\dfrac {\d y} {\d x} + \dfrac y x = 3 x$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$x y = x^3 + C$ or: :$y = x^2 + \dfrac C x$
This is a special case of: :[[Linear First Order ODE/y' + (y over x) = k x^n|Linear First Order ODE: $\dfrac {\d y} {\d x} + \dfrac y x = k x^n$]] where $k = 3$ and $n = 1$, yielding: :$y = x^2 + \dfrac C x$ Multiplying through by $x$ reveals: :$x y = x^3 + C$ {{qed}}
Linear First Order ODE/y' + (y over x) = 3 x
https://proofwiki.org/wiki/Linear_First_Order_ODE/y'_+_(y_over_x)_=_3_x
https://proofwiki.org/wiki/Linear_First_Order_ODE/y'_+_(y_over_x)_=_3_x
[ "Examples of Linear First Order ODEs" ]
[ "Definition:Linear First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Linear First Order ODE/y' + (y over x) = k x^n" ]
proofwiki-10996
Linear First Order ODE/x y' - 3 y = x^4
The linear first order ODE: :$(1): \quad x \dfrac {\d y} {\d x} - 3y = x^4$ has the general solution: :$y = x^4 + \dfrac C {x^3}$
Rearranging $(1)$: :$(2): \quad \dfrac {\d y} {\d x} + \paren {-\dfrac 3 x} y = x^3$ $(2)$ is a linear first order ODE in the form: :$\dfrac {\d y} {\d x} + \map P x y = \map Q x$ where: :$\map P x = -\dfrac 3 x$ :$\map Q x = x^3$ Thus: {{begin-eqn}} {{eqn | l = \int \map P x \rd x | r = \int -\frac 3 x \rd x ...
The [[Definition:Linear First Order ODE|linear first order ODE]]: :$(1): \quad x \dfrac {\d y} {\d x} - 3y = x^4$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$y = x^4 + \dfrac C {x^3}$
Rearranging $(1)$: :$(2): \quad \dfrac {\d y} {\d x} + \paren {-\dfrac 3 x} y = x^3$ $(2)$ is a [[Definition:Linear First Order ODE|linear first order ODE]] in the form: :$\dfrac {\d y} {\d x} + \map P x y = \map Q x$ where: :$\map P x = -\dfrac 3 x$ :$\map Q x = x^3$ Thus: {{begin-eqn}} {{eqn | l = \int \map P x \...
Linear First Order ODE/x y' - 3 y = x^4
https://proofwiki.org/wiki/Linear_First_Order_ODE/x_y'_-_3_y_=_x^4
https://proofwiki.org/wiki/Linear_First_Order_ODE/x_y'_-_3_y_=_x^4
[ "Examples of Linear First Order ODEs" ]
[ "Definition:Linear First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Linear First Order Ordinary Differential Equation", "Solution to Linear First Order Ordinary Differential Equation/Solution by Integrating Factor", "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10997
Linear First Order ODE/y' + y = 1 over (1 + exp 2 x)
The linear first order ODE: :$(1): \quad y' + y = \dfrac 1 {1 + e^{2 x} }$ has the general solution: :$y = e^{-x} \map \arctan {e^x} + C e^{-x}$
$(1)$ is in the form: :$\dfrac {\d y} {\d x} + \map P x y = \map Q x$ where $\map P x = 1$. Thus: {{begin-eqn}} {{eqn | l = \int \map P x \rd x | r = \int \rd x | c = }} {{eqn | r = x | c = }} {{eqn | ll= \leadsto | l = e^{\int P \rd x} | r = e^x | c = }} {{end-eqn}} Thus from Sol...
The [[Definition:Linear First Order ODE|linear first order ODE]]: :$(1): \quad y' + y = \dfrac 1 {1 + e^{2 x} }$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$y = e^{-x} \map \arctan {e^x} + C e^{-x}$
$(1)$ is in the form: :$\dfrac {\d y} {\d x} + \map P x y = \map Q x$ where $\map P x = 1$. Thus: {{begin-eqn}} {{eqn | l = \int \map P x \rd x | r = \int \rd x | c = }} {{eqn | r = x | c = }} {{eqn | ll= \leadsto | l = e^{\int P \rd x} | r = e^x | c = }} {{end-eqn}} Thus from [...
Linear First Order ODE/y' + y = 1 over (1 + exp 2 x)
https://proofwiki.org/wiki/Linear_First_Order_ODE/y'_+_y_=_1_over_(1_+_exp_2_x)
https://proofwiki.org/wiki/Linear_First_Order_ODE/y'_+_y_=_1_over_(1_+_exp_2_x)
[ "Examples of Linear First Order ODEs" ]
[ "Definition:Linear First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Solution to Linear First Order Ordinary Differential Equation/Solution by Integrating Factor", "Definition:Differential Equation/Solution/General Solution", "Primitive of Reciprocal of x squared plus a squared/Arctangent Form" ]
proofwiki-10998
Linear First Order ODE/(1 + x^2) dy + 2 x y dx = cotangent x dx
The linear first order ODE: :$(1): \quad \paren {1 + x^2} \rd y + 2 x y \rd x = \cot x \rd x$ has the general solution: :$y = \dfrac {\map \ln {\sin x} } {1 + x^2} + \dfrac C {1 + x^2}$
$(1)$ can be written as: :$(2): \quad \paren {1 + x^2} \dfrac {\rd y} {\rd x} + 2 x y = \cot x$ We notice straight away that: :$\dfrac {\rd} {\rd x} \paren {1 + x^2} = 2 x$ and so: :$\dfrac {\rd} {\rd x} \paren {1 + x^2} y = \cot x$ Thus the general solution becomes: {{begin-eqn}} {{eqn | l = \paren {1 + x^2} y |...
The [[Definition:Linear First Order ODE|linear first order ODE]]: :$(1): \quad \paren {1 + x^2} \rd y + 2 x y \rd x = \cot x \rd x$ has the [[Definition:General Solution to Differential Equation|general solution]]: :$y = \dfrac {\map \ln {\sin x} } {1 + x^2} + \dfrac C {1 + x^2}$
$(1)$ can be written as: :$(2): \quad \paren {1 + x^2} \dfrac {\rd y} {\rd x} + 2 x y = \cot x$ We notice straight away that: :$\dfrac {\rd} {\rd x} \paren {1 + x^2} = 2 x$ and so: :$\dfrac {\rd} {\rd x} \paren {1 + x^2} y = \cot x$ Thus the [[Definition:General Solution to Differential Equation|general solution]] ...
Linear First Order ODE/(1 + x^2) dy + 2 x y dx = cotangent x dx
https://proofwiki.org/wiki/Linear_First_Order_ODE/(1_+_x^2)_dy_+_2_x_y_dx_=_cotangent_x_dx
https://proofwiki.org/wiki/Linear_First_Order_ODE/(1_+_x^2)_dy_+_2_x_y_dx_=_cotangent_x_dx
[ "Examples of Linear First Order ODEs" ]
[ "Definition:Linear First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Definition:Differential Equation/Solution/General Solution" ]
proofwiki-10999
Linear First Order ODE/y' + y = 2 x exp -x + x^2
The linear first order ODE: :$(1): \quad y' + y = 2 x e^{-x} + x^2$ has the general solution: :$y = x^2 e^{-x} + x^2 - 2 x + 2 + C e^{-x}$
$(1)$ is in the form: :$\dfrac {\d y} {\d x} + \map P x y = \map Q x$ where: :$\map P x = 1$ Thus: {{begin-eqn}} {{eqn | l = \int \map P x \rd x | r = \int 1 \rd x | c = }} {{eqn | r = x | c = }} {{eqn | ll= \leadsto | l = e^{\int P \rd x} | r = e^x | c = }} {{end-eqn}} Thus from ...
The [[Definition:Linear First Order ODE|linear first order ODE]]: :$(1): \quad y' + y = 2 x e^{-x} + x^2$ has the [[Definition:General Solution of Differential Equation|general solution]]: :$y = x^2 e^{-x} + x^2 - 2 x + 2 + C e^{-x}$
$(1)$ is in the form: :$\dfrac {\d y} {\d x} + \map P x y = \map Q x$ where: :$\map P x = 1$ Thus: {{begin-eqn}} {{eqn | l = \int \map P x \rd x | r = \int 1 \rd x | c = }} {{eqn | r = x | c = }} {{eqn | ll= \leadsto | l = e^{\int P \rd x} | r = e^x | c = }} {{end-eqn}} Thus fro...
Linear First Order ODE/y' + y = 2 x exp -x + x^2
https://proofwiki.org/wiki/Linear_First_Order_ODE/y'_+_y_=_2_x_exp_-x_+_x^2
https://proofwiki.org/wiki/Linear_First_Order_ODE/y'_+_y_=_2_x_exp_-x_+_x^2
[ "Examples of Linear First Order ODEs" ]
[ "Definition:Linear First Order Ordinary Differential Equation", "Definition:Differential Equation/Solution/General Solution" ]
[ "Solution to Linear First Order Ordinary Differential Equation/Solution by Integrating Factor", "Definition:Differential Equation/Solution/General Solution" ]