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

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Page 106

We can summarize our remarks as follows: Each possible quantum state of a

system can be specified by some set off

the number of degrees of freedom of the system, is equal to the number of ...

We can summarize our remarks as follows: Each possible quantum state of a

system can be specified by some set off

**quantum numbers**. This number f. calledthe number of degrees of freedom of the system, is equal to the number of ...

Page 121

In the i.e., it is simply equal to the volume of “number space" defined by three

perpendicular axes labeled by n, ny, n., the possible values of these three

length, ...

In the i.e., it is simply equal to the volume of “number space" defined by three

perpendicular axes labeled by n, ny, n., the possible values of these three

**quantum numbers**lie thus geometrically at the centers of cubes of unit edgelength, ...

Page 122

(6) oc (e — eo)" where a ~ 1, (33) i.e., where o is some number of the order of

unity.t Consider now the entire system with f ... (6) possible values which can be

assumed by the 1st of its

(6) oc (e — eo)" where a ~ 1, (33) i.e., where o is some number of the order of

unity.t Consider now the entire system with f ... (6) possible values which can be

assumed by the 1st of its

**quantum numbers**, q(e) possible values which can be ...### What people are saying - Write a review

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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