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

### From inside the book

Results 1-3 of 12

Page 210

This can be done by placing the system in successive contacts with a series of

heat reservoirs of infinitesimally different ... (30) If the

independent of temperature in the temperature range between Ta and To, (30)

becomes ...

This can be done by placing the system in successive contacts with a series of

heat reservoirs of infinitesimally different ... (30) If the

**heat capacity**C, isindependent of temperature in the temperature range between Ta and To, (30)

becomes ...

Page 218

5.12

magnetic moment u0, is located in an external magnetic field B and is in

equilibrium at the absolute temperature T. Focus attention on the spins only and

answer ...

5.12

**Heat capacity**of a spin system A system of N atoms, each having spin + andmagnetic moment u0, is located in an external magnetic field B and is in

equilibrium at the absolute temperature T. Focus attention on the spins only and

answer ...

Page 220

If such a metal is superconducting below a critical temperature T., then its

approximately given by the relation C. = o(To where a is some constant. No heat

is ...

If such a metal is superconducting below a critical temperature T., then its

**heat****capacity**C, in the superconducting state in the temperature range 0 < T K T. isapproximately given by the relation C. = o(To where a is some constant. No heat

is ...

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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