## Fundamentals of statistical and thermal physics |

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Page 375

9'13-1 The energy density u(ij) (per unit dimensionless frequency range dri) as a

function of ti = hw/kT.

,. ELECTROMAGNETIC RADIATION IN THERMAL EQUILIBRIUM S76.

9'13-1 The energy density u(ij) (per unit dimensionless frequency range dri) as a

function of ti = hw/kT.

**perature**T\ the maximum occurs at the angular frequency Ģi,. ELECTROMAGNETIC RADIATION IN THERMAL EQUILIBRIUM S76.

Page 376

temperature Ti the maximum occurs at a>2, then one must have hu>i _ hui _ . (

913 13) This result is known as "Wien's displacement law." The mean total

energy ...

**perature**T\ the maximum occurs at the angular frequency Ģi, and at some othertemperature Ti the maximum occurs at a>2, then one must have hu>i _ hui _ . (

913 13) This result is known as "Wien's displacement law." The mean total

energy ...

Page 451

... all fields H and to find the quantity (dT/dH)s in (11 -2 - 10). tem- n by Example

As a very special case, suppose that in a certain range of

field the susceptibility x is approximately given Curie's law a where a is constant.

... all fields H and to find the quantity (dT/dH)s in (11 -2 - 10). tem- n by Example

As a very special case, suppose that in a certain range of

**perature**and magneticfield the susceptibility x is approximately given Curie's law a where a is constant.

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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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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