## Fundamentals of statistical and thermal physics |

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Page 79

Clearly dF in (2 111) is simply the infinitesimal difference between two adjacent

values of the function F. The infinitesimal

differential; it is also called an "exact differential" to distinguish it from other kinds

of ...

Clearly dF in (2 111) is simply the infinitesimal difference between two adjacent

values of the function F. The infinitesimal

**quantity**dF is here just an ordinarydifferential; it is also called an "exact differential" to distinguish it from other kinds

of ...

Page 149

The internal energy E of a system is an extensive

required to subdivide the system into two parts (if one neglects the work involved

in creating the two new surfaces; this is negligible for large systems for which the

...

The internal energy E of a system is an extensive

**quantity**. Indeed, no work isrequired to subdivide the system into two parts (if one neglects the work involved

in creating the two new surfaces; this is negligible for large systems for which the

...

Page 168

Here the

is simply the change of volume with temperature under conditions of constant

pressure. Indeed, one defines the intensive

...

Here the

**quantity**on the right is a readily measured and familiar**quantity**, since itis simply the change of volume with temperature under conditions of constant

pressure. Indeed, one defines the intensive

**quantity**(5-7-8) (5-7-9) - 1 fdV\ as 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