## Statistical Physics, Volume 5Elementary college physics course for students majoring in science and engineering. |

### From inside the book

Results 1-3 of 6

Page 126

Example Suppose that the partition in Fig. 3.8 is (...) (...) - - - (...) - (#) removed.

This leaves the total energy V, / \V, V. J T \V, ) of the gas unchanged, but

eliminates the N terms former constraint that prevented mole.

occupying the ...

Example Suppose that the partition in Fig. 3.8 is (...) (...) - - - (...) - (#) removed.

This leaves the total energy V, / \V, V. J T \V, ) of the gas unchanged, but

eliminates the N terms former constraint that prevented mole.

**cules**fromoccupying the ...

Page 232

the container is thus independent of the position vector r of the molecule. The

state of the molecule is described classically in terms of the three position ...

**cules**is supposed to be negligible. The energy of the molecule anywhere withinthe container is thus independent of the position vector r of the molecule. The

state of the molecule is described classically in terms of the three position ...

Page 336

... Since the total number of labeled molecules is conserved, we can make the

statement that (the increase per unit This equation expresses merely the

conservation of the number of labeled moletime in the number of labeled

molecules

... Since the total number of labeled molecules is conserved, we can make the

statement that (the increase per unit This equation expresses merely the

conservation of the number of labeled moletime in the number of labeled

molecules

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### 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