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College_Physics_2e-WEB_7Zesafu_chunk_2099 | planets in our solar system, for example, may be chaotic (we are not certain yet). But they are definitely organized
and systematic, with a simple formula describing the orbital radii of the first eight planets and the asteroid belt.
Large-scale vortices in Jupiter’s atmosphere are chaotic, but the Great Red Spot is a ... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2100 | The emerging field of complexity, like the now almost traditional field of chaos, is partly rooted in physics. Both
attempt to see similar systematics in a very broad range of phenomena and, hence, generate a better understanding
of them. Time will tell what impact these fields have on more traditional areas of physics... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2101 | and was surprised to observe the resistivity of a mediocre conductor like mercury drop to zero at a temperature of
4.2 K. We define the temperature at which and below which a material becomes a superconductor to be its critical
temperature, denoted by
. (See Figure 34.23.) Progress in understanding how and why a materi... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2102 | found to become superconductors, but all had
s less than 10 K, which are expensive to maintain. Although Onnes
received a Nobel prize in 1913, it was primarily for his work with liquid helium.
In 1986, a breakthrough was announced—a ceramic compound was found to have an unprecedented
of 35 K. It
looked as if much highe... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2103 | temperature (about 293 K) would be ideal, but any temperature close to room temperature is relatively cheap to
produce and maintain. There are persistent reports of
s over 200 K and some in the vicinity of 270 K.
Unfortunately, these observations are not routinely reproducible, with samples losing their superconducting... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2104 | losing energy to it, making it a superconductor. High-
superconductors are more difficult to understand
theoretically, but theorists seem to be closing in on a workable theory. The difficulty of understanding how electrons
can sneak through materials without losing energy in collisions is even greater at higher tempera... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2105 | if answers are found to them. The fun continues.
On the Largest Scale
1.
Is the universe open or closed? Theorists would like it to be just barely closed and evidence is building toward
that conclusion. Recent measurements in the expansion rate of the universe and in CMBR support a flat
universe. There is a connection ... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2106 | interactions or black holes eating a companion neutron star can be explored.
On the Intermediate Scale
1.
How do phase transitions take place on the microscopic scale? We know a lot about phase transitions, such as
water freezing, but the details of how they occur molecule by molecule are not well understood. Similar
q... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2107 | want them to be. The answer may have to be indirectly obtained because of the extreme energy at which we
think they are unified.
5.
Are there other fundamental forces? There was a flurry of activity with claims of a fifth and even a sixth force a
few years ago. Interest has subsided, since those forces have not been de... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2108 | Glossary
axions
a type of WIMPs having masses about 10−10
of an electron mass
Big Bang
a gigantic explosion that threw out matter a
few billion years ago
black holes
objects having such large gravitational
fields that things can fall in, but nothing, not even
light, can escape
chaos
word used to describe systems the ou... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2109 | between us and the star
negatively curved
an open universe that expands
forever
neutralinos
a type of WIMPs having masses several
orders of magnitude greater than nucleon masses
neutrino oscillations
a process in which any type of
neutrino could change spontaneously into any other
neutron stars
literally a star compose... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2110 | •
Galaxies farther away than our local group have,
on an average, a recessional velocity given by
where
is the distance to the galaxy and
is the
Hubble constant, taken to have the average value
•
Explanations of the large-scale characteristics of
the universe are intimately tied to particle physics.
•
The dominance of ... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2111 | predicted by general relativity but not yet
observed, caused by changes in very massive
objects.
•
Quantum gravity is an incompletely developed
theory that strives to include general relativity,
quantum mechanics, and unification of forces
(thus, a TOE).
•
One unconfirmed connection between general
relativity and quant... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2112 | other disciplines, such as biological evolution.
•
Chaos is a field that studies systems whose
properties depend extremely sensitively on some
variables and whose evolution is impossible to
predict.
•
Chaotic systems may be simple or complex.
•
Studies of chaos have led to methods for
understanding and predicting certa... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2113 | eventually fall on a star’s surface. Why then is the
sky dark at night? Discuss the commonly accepted
evolution of the universe as a solution to this
paradox.
7. If the cosmic microwave background radiation
(CMBR) is the remnant of the Big Bang’s fireball, we
expect to see hot and cold regions in it. What are
two cause... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2114 | 34.2 General Relativity and Quantum
Gravity
12. Quantum gravity, if developed, would be an
improvement on both general relativity and
quantum mechanics, but more mathematically
difficult. Under what circumstances would it be
necessary to use quantum gravity? Similarly,
under what circumstances could general relativity
... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2115 | 21. Lacking direct evidence of WIMPs as dark matter,
why must we eliminate all other possible
explanations based on the known forms of matter
before we invoke their existence?
34.5 Complexity and Chaos
22. Must a complex system be adaptive to be of
interest in the field of complexity? Give an
example to support your an... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2116 | Problems & Exercises
34.1 Cosmology and Particle Physics
1. Find the approximate mass of the luminous matter
in the Milky Way galaxy, given it has approximately
stars of average mass 1.5 times that of our
Sun.
2. Find the approximate mass of the dark and
luminous matter in the Milky Way galaxy. Assume
the luminous matt... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2117 | it would take to travel 1 Mly at a constant expansion
rate of 20 km/s. (b) If deceleration is taken into
account, would the actual age of the universe be
greater or less than that found here? Explain.
9. Assuming a circular orbit for the Sun about the
center of the Milky Way galaxy, calculate its orbital
speed using th... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2118 | such photons.
(c) If the average massive particle in space has a
mass half that of a proton, what energy would be
created by converting its mass to energy? (d) Does
this imply that space is “matter dominated”?
Explain briefly.
15. (a) What Hubble constant corresponds to an
approximate age of the universe of
y? To get
a... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2119 | 16. Show that the velocity of a star orbiting its galaxy
in a circular orbit is inversely proportional to the
square root of its orbital radius, assuming the
mass of the stars inside its orbit acts like a single
mass at the center of the galaxy. You may use an
equation from a previous chapter to support your
conclusion... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2120 | that has a mass eight times that of our Sun? Note
that stars must be more massive than the Sun to
form black holes as a result of a supernova.
23. Black holes with masses smaller than those
formed in supernovas may have been created in
the Big Bang. Calculate the radius of one that has
a mass equal to the Earth’s.
24. ... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2121 | 25. Construct Your Own Problem
Consider a supermassive black hole near the
center of a galaxy. Calculate the radius of such an
object based on its mass. You must consider how
much mass is reasonable for these large objects,
and which is now nearly directly observed.
(Information on black holes posted on the Web by
NASA... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2122 | 34.6 High-temperature Superconductors
31. A section of superconducting wire carries a
current of 100 A and requires 1.00 L of liquid
nitrogen per hour to keep it below its critical
temperature. For it to be economically
advantageous to use a superconducting wire, the
cost of cooling the wire must be less than the cost
... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2123 | APPENDIX A
Atomic Masses
Atomic
Number,
Z
Name
Atomic Mass
Number, A
Symbol
Atomic
Mass (u)
Percent Abundance
or Decay Mode
Half-life, t1/2
0
neutron
1
1.008
665
10.37 min
1
Hydrogen
1
1.007
825
99.985%
Deuterium
2
2.014
102
0.015%
Tritium
3
3.016
050
12.33 y
2
Helium
3
3.016
030
4
4.002
603
3
Lithium
6
6.015
121
7.5%
... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2124 | Atomic
Number,
Z
Name
Atomic Mass
Number, A
Symbol
Atomic
Mass (u)
Percent Abundance
or Decay Mode
Half-life, t1/2
12
Magnesium
24
23.985
042
78.99%
13
Aluminum
27
26.981
539
100%
14
Silicon
28
27.976
927
92.23%
2.62h
31
30.975
362
15
Phosphorus
31
30.973
762
100%
32
31.973
907
14.28 d
16
Sulfur
32
31.972
070
95.02%
35... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2125 | Atomic
Number,
Z
Name
Atomic Mass
Number, A
Symbol
Atomic
Mass (u)
Percent Abundance
or Decay Mode
Half-life, t1/2
74
73.921
177
36.5%
33
Arsenic
75
74.921
594
100%
34
Selenium
80
79.916
520
49.7%
35
Bromine
79
78.918
336
50.69%
36
Krypton
84
83.911
507
57.0%
37
Rubidium
85
84.911
794
72.17%
38
Strontium
86
85.909
267
... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2126 | Atomic
Number,
Z
Name
Atomic Mass
Number, A
Symbol
Atomic
Mass (u)
Percent Abundance
or Decay Mode
Half-life, t1/2
134
133.906
696
EC,
2.06 y
56
Barium
137
136.905
812
11.23%
138
137.905
232
71.70%
57
Lanthanum
139
138.906
346
99.91%
58
Cerium
140
139.905
433
88.48%
59
Praseodymium
141
140.907
647
100%
60
Neodymium
142... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2127 | Atomic
Number,
Z
Name
Atomic Mass
Number, A
Symbol
Atomic
Mass (u)
Percent Abundance
or Decay Mode
Half-life, t1/2
202
201.970
617
29.86%
81
Thallium
205
204.974
401
70.48%
82
Lead
206
205.974
440
24.1%
207
206.975
872
22.1%
208
207.976
627
52.4%
210
209.984
163
22.3 y
211
210.988
735
36.1 min
212
211.991
871
10.64 h
8... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2128 | Atomic
Number,
Z
Name
Atomic Mass
Number, A
Symbol
Atomic
Mass (u)
Percent Abundance
or Decay Mode
Half-life, t1/2
99
Einsteinium
254
254.088
019
276 d
100
Fermium
253
253.085
173
EC,
3.00 d
101
Mendelevium
255
255.091
081
EC,
27 min
102
Nobelium
255
255.093
260
EC,
3.1 min
103
Lawrencium
257
257.099
480
EC,
0.646 s
10... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2129 | Isotope
t 1/2
DecayMode(s)
Energy(MeV)
Percent
-Ray
Energy(MeV)
Percent
1.33
100%
244.1 d
EC
1.12
51%
78.3 h
EC
0.0933
70%
0.185
35%
0.300
19%
others
118.5 d
EC
0.121
20%
0.136
65%
0.265
68%
0.280
20%
others
18.8 d
0.69
9%
1.08
9%
1.77
91%
64.8 d
EC
0.514
100%
28.8 y
0.546
100%
64.1 h
2.28
100%
6.02 h
IT
0.142
100%
99.... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2130 | Isotope
t 1/2
DecayMode(s)
Energy(MeV)
Percent
-Ray
Energy(MeV)
Percent
5.32
11%
others
TABLE B1 Selected Radioactive Isotopes
1552
B • Selected Radioactive Isotopes
Access for free at openstax.org
APPENDIX C
Useful Information
This appendix is broken into several tables.
•
Table C1, Important Constants
•
Table C2, Su... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2131 | Prefix
Symbol
Value
Prefix
Symbol
Value
deka
da
pico
p
—
—
femto
f
TABLE C4 Metric Prefixes for Powers of Ten and Their
Symbols
Alpha
Eta
Nu
Tau
Beta
Theta
Xi
Upsilon
Gamma
Iota
Omicron
Phi
Delta
Kappa
Pi
Chi
Epsilon
Lambda
Rho
Psi
Zeta
Mu
Sigma
Omega
TABLE C5 The Greek Alphabet
Entity
Abbreviation
Name
Fundamental uni... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2132 | Symbol
Definition
change in energy between the initial and final orbits of an electron in an atom
uncertainty in energy
difference in mass between initial and final products
number of decays that occur
change in momentum
uncertainty in momentum
change in gravitational potential energy
rotation angle
distance traveled a... | College_Physics_2e-WEB_7Zesafu | pdf |
College_Physics_2e-WEB_7Zesafu_chunk_2133 | Symbol
Definition
center of mass
quark flavor charm
specific heat
speed of light
kilocalorie
calorie
heat pump’s coefficient of performance
coefficient of performance for refrigerators and air conditioners
cosine
cotangent
cosecant
diffusion constant
displacement
quark flavor down
decibel
distance of an image from the ... | College_Physics_2e-WEB_7Zesafu | pdf |
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