## Fundamentals of statistical and thermal physics |

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Page 129

The determination of the

a measurement of macroscopic work. If one considers a system which is

thermally insulated so that it cannot absorb any heat, then Q = 0 and one has

simply ħE ...

The determination of the

**internal energy**E of a system is, by (311-2), reducible toa measurement of macroscopic work. If one considers a system which is

thermally insulated so that it cannot absorb any heat, then Q = 0 and one has

simply ħE ...

Page 153

The first law (311-2) applied to any infinitesimal process yields the relation dQ =

dE + dW where dE is the change of

consideration. If the process is quasi-static, the second law (311-2) allows one to

express ...

The first law (311-2) applied to any infinitesimal process yields the relation dQ =

dE + dW where dE is the change of

**internal energy**of the system underconsideration. If the process is quasi-static, the second law (311-2) allows one to

express ...

Page 228

Consider the case where A can exchange both energy and momentum with the

much larger system A'. If A is in a state ... The number of states Sl'(E') accessible

to A' depends on its

...

Consider the case where A can exchange both energy and momentum with the

much larger system A'. If A is in a state ... The number of states Sl'(E') accessible

to A' depends on its

**internal energy**E' with respect to its center of mass. Since 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