## Fundamentals of statistical and thermal physics |

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Page 75

In particular, when the parameters are changed by infinitesimal amounts so that

xa — * xa + dxa for each a, then (2-9-1) gives for the

energy V* dE. - 1 dEr= 2 ^dx- (2-9-2) a-l " The work dW done by the system when

it ...

In particular, when the parameters are changed by infinitesimal amounts so that

xa — * xa + dxa for each a, then (2-9-1) gives for the

**corresponding**change inenergy V* dE. - 1 dEr= 2 ^dx- (2-9-2) a-l " The work dW done by the system when

it ...

Page 309

(The points on this curve are labeled to

this diagram one can readily see what happens for various values of the pressure

. At 0 only the high-compressibility phase (in our example, the gas) exists.

(The points on this curve are labeled to

**correspond**to those of Fig. 8-6-2.) Fromthis diagram one can readily see what happens for various values of the pressure

. At 0 only the high-compressibility phase (in our example, the gas) exists.

Page 368

3C( denotes the Hamiltonian describing the translational motion of the center of

mass of the molecule; tt(st) denotes the

translational state labeled st. 3Ce denotes the Hamiltonian describing the ...

3C( denotes the Hamiltonian describing the translational motion of the center of

mass of the molecule; tt(st) denotes the

**corresponding**translational energy of thetranslational state labeled st. 3Ce denotes the Hamiltonian describing the ...

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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