Statistical Physics, Volume 5Elementary college physics course for students majoring in science and engineering. |
From inside the book
Results 1-3 of 81
Page 64
2.2 Elementary Relations among Probabilities Probabilities satisfy some simple
relations which are almost selfevident, but quite important. It will be worth
deriving these relations by starting directly from the definition (1) of a probability.
2.2 Elementary Relations among Probabilities Probabilities satisfy some simple
relations which are almost selfevident, but quite important. It will be worth
deriving these relations by starting directly from the definition (1) of a probability.
Page 184
(b) Use (i) to calculate the mean energy E of the gas by means of the general
relation derived in Prob. 4.18. Show that the functional form of (i) implies
immediately that E must be simply N times as large as the mean energy per
molecule.
(b) Use (i) to calculate the mean energy E of the gas by means of the general
relation derived in Prob. 4.18. Show that the functional form of (i) implies
immediately that E must be simply N times as large as the mean energy per
molecule.
Page 270
Note that this relation allows us to calculate the mean pressure exerted by a
system if its entropy is known as a function of its volume. We derived the relation (
13) by considering how the energy levels of the system move in or out of a given
...
Note that this relation allows us to calculate the mean pressure exerted by a
system if its entropy is known as a function of its volume. We derived the relation (
13) by considering how the energy levels of the system move in or out of a given
...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Characteristic Features of Macroscopic Systems | 1 |
A I | 2 |
I | 6 |
Copyright | |
26 other sections not shown
Common terms and phrases
absolute temperature absorbed accessible approximation assume atoms average Avogadro's calculate classical collision Consider constant container corresponding cules denote discussion distribution ensemble entropy equal equilibrium situation equipartition theorem example exchange energy expression external parameters fluctuations function given heat capacity heat Q heat reservoir Hence ideal gas initial internal energy interval isolated system kinetic energy large number left half liquid ln Q macroscopic parameters macroscopic system macrostate magnetic field magnetic moment magnitude mass mean energy mean number mean pressure mean value measured mechanics mole molecular momentum number of molecules occur oscillator particle particular partition phase space piston position possible values Prob quantity quantum numbers quasi-static random relation result simply solid specific heat spin system statistical statistical ensemble statistically independent Suppose thermal contact thermal interaction thermally insulated thermometer tion total energy total magnetic total number unit volume velocity