## Fundamentals of statistical and thermal physics |

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Page 211

Another situation of physical interest is that where a system A consists of a fixed

number N of particles in a given volume V, but where the only information

available about the energy of the system is its

common ...

Another situation of physical interest is that where a system A consists of a fixed

number N of particles in a given volume V, but where the only information

available about the energy of the system is its

**mean energy**E. This is a verycommon ...

Page 212

Rather, it is to be determined by the condition that the

with the distribution (6 • 4 • 2) is indeed equal to the specified mean value E, i.e.,

by the condition £ er"'Er (6-4-3) In short, when one is dealing with a system in ...

Rather, it is to be determined by the condition that the

**mean energy**calculatedwith the distribution (6 • 4 • 2) is indeed equal to the specified mean value E, i.e.,

by the condition £ er"'Er (6-4-3) In short, when one is dealing with a system in ...

Page 227

E,-aNrET (6-9-5) R = ^ £ e-0Br-aNr r Here the sums are over all possible states of

the system A irrespective of its number of particles or of its energy. When A is a ...

**mean energy**E and mean number ft of particles, i.e., by the equations E = \ V e-»E,-aNrET (6-9-5) R = ^ £ e-0Br-aNr r Here the sums are over all possible states of

the system A irrespective of its number of particles or of its energy. When A is a ...

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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 | |

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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