Fundamentals of Statistical and Thermal Physics, Volume 10This book is devoted to a discussion of some of the basic physical concepts and methods useful in the description of situations involving systems which consist of very many particulars. It attempts, in particular, to introduce the reader to the disciplines of thermodynamics, statistical mechanics, and kinetic theory from a unified and modern point of view. The presentation emphasizes the essential unity of the subject matter and develops physical insight by stressing the microscopic content of the theory. |
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Results 1-3 of 87
Page 183
... ideal gas = 0. If n is not too large , only the first few terms in ( 5-10-12 ) are important . The first correction to the ideal gas consists of retaining the term B2n2 and neglecting all higher - order terms . ( 5-10-12 ) becomes B2 ...
... ideal gas = 0. If n is not too large , only the first few terms in ( 5-10-12 ) are important . The first correction to the ideal gas consists of retaining the term B2n2 and neglecting all higher - order terms . ( 5-10-12 ) becomes B2 ...
Page 282
... Gases , " chaps . 2 and 5 , McGraw - Hill Book Com- pany , New York , 1958 . PROBLEMS 7.1 Consider a homogeneous mixture of inert monatomic ideal gases at absolute temperature T in a container of volume V. Let there be v1 moles of gas 1 ...
... Gases , " chaps . 2 and 5 , McGraw - Hill Book Com- pany , New York , 1958 . PROBLEMS 7.1 Consider a homogeneous mixture of inert monatomic ideal gases at absolute temperature T in a container of volume V. Let there be v1 moles of gas 1 ...
Page 398
... ideal FD gas . Express your answer solely in terms of ñ ,, the mean number of particles in state r . ( b ) Write a similar expression for the entropy S of a BE gas . ( c ) What do these expressions for S become in the classical limit ...
... ideal FD gas . Express your answer solely in terms of ñ ,, the mean number of particles in state r . ( b ) Write a similar expression for the entropy S of a BE gas . ( c ) What do these expressions for S become in the classical limit ...
Contents
Introduction to statistical methods | 1 |
GENERAL DISCUSSION OF THE RANDOM WALK | 24 |
Statistical description of systems of particles | 47 |
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absolute temperature approximation assume atoms becomes Boltzmann equation calculate chemical potential classical coefficient collision condition Consider constant container corresponding curve d³r d³v denote density depends discussion e-BE electrons ensemble entropy equal equation equilibrium situation equipartition theorem evaluated example expression external parameters fluctuations gases given heat capacity heat reservoir Hence ideal gas independent infinitesimal integral integrand interaction internal energy isolated system kinetic liquid macroscopic macrostate magnetic field magnetic moment mass maximum mean energy mean number mean pressure mean value mole molecular molecules momentum n₁ number of molecules number of particles obtains partition function phase space photons physical piston probability problem quantity quantum quantum mechanics quasi-static range relation result simply solid specific heat spin statistical mechanics thermal contact thermally insulated Thermodynamics tion total number unit volume v₁ variables velocity