## Fundamentals of statistical and thermal physics |

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Page 102

If two systems separately in equilibrium are characterized by the same value of

the parameter, then the systems will remain in equilibrium when brought into

values ...

If two systems separately in equilibrium are characterized by the same value of

the parameter, then the systems will remain in equilibrium when brought into

**thermal contact**with each other. 2. If the systems are characterized by differentvalues ...

Page 104

If the thermometric parameter of M does not have the same value in both cases,

then one knows that A and B will not remain in equilibrium if brought into

...

If the thermometric parameter of M does not have the same value in both cases,

then one knows that A and B will not remain in equilibrium if brought into

**thermal****contact**with each other. For suppose they did remain in equilibrium; then, after M...

Page 445

The gas is initially in

a water bath. One can now compress the gas to a volume V,-. In this process

work is done on the gas, but it can give off heat to the bath and thus remains at

the ...

The gas is initially in

**thermal contact**with a heat bath at temperature T„ e.g., witha water bath. One can now compress the gas to a volume V,-. In this process

work is done on the gas, but it can give off heat to the bath and thus remains at

the ...

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#### LibraryThing Review

User Review - JJMAlmeida - LibraryThingNever mind that this book was published in the mid '60s (before I was even born); if you must choose one book to learn from, choose this one. It is so concise, so well thought out that I have yet to ... Read full review

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i want this book

Reif: fundamental of statistical thermal physics

### Contents

Introduction to statistical methods | 1 |

GENERAL DISCUSSION OF THE RANDOM WALK | 24 |

Statistical description of systems of particles | 47 |

Copyright | |

24 other sections not shown

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### Common terms and phrases

absolute temperature approximation assume atoms becomes Boltzmann equation calculate canonical distribution chemical potential classical coefficient collision condition Consider constant container corresponding curve denote density depends derivatives discussion electrons ensemble entropy equal equation equilibrium situation equipartition theorem evaluated example expression external parameters fluctuations frequency gases given heat capacity heat reservoir Hence ideal gas independent infinitesimal integral integrand interaction internal energy isolated system kinetic liquid macroscopic macrostate magnetic field mass maximum mean energy mean number mean pressure mean value measured metal molar mole molecular momentum number of molecules number of particles obtains partition function perature phase space photons physical piston position probability problem quantity quantum quantum mechanics quasi-static radiation range relation result simply solid specific heat spin statistical mechanics Suppose theorem thermal contact thermally insulated Thermodynamics tion total energy total number unit volume variables velocity yields