## Fundamentals of statistical and thermal physics |

### From inside the book

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Page 201

Our aim will be (1) to derive general probability statements for a variety of

situations of

macroscopic quantities (such as entropies or specific heats) from a knowledge of

the ...

Our aim will be (1) to derive general probability statements for a variety of

situations of

**physical**interest and (2) to describe practical methods for calculatingmacroscopic quantities (such as entropies or specific heats) from a knowledge of

the ...

Page 214

To show this explicitly, we recall that Z in (6 • 5 □ 3) is a function of both * The

situation is completely analogous to that encountered in (3 • 12 • 1), where all

consequence ...

To show this explicitly, we recall that Z in (6 • 5 □ 3) is a function of both * The

situation is completely analogous to that encountered in (3 • 12 • 1), where all

**physical**quantities could be expressed in terms of In SI. The**physical**consequence ...

Page 532

electrical conductivity which, although almost as simple as the elementary

arguments of Chapter 12, will bring out several new features of

significance. Consider the case of ions of mass m and charge e which move in a

neutral gas ...

electrical conductivity which, although almost as simple as the elementary

arguments of Chapter 12, will bring out several new features of

**physical**significance. Consider the case of ions of mass m and charge e which move in a

neutral gas ...

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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