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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Page 183
... ideal gas B2 = B3 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 . In this case ( 5.10 ...
... ideal gas B2 = B3 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 . In this case ( 5.10 ...
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 . ň , ( b ) Write a similar expression for the entropy S of a BE gas . ( c ) What do these expressions for S become in the classical ...
... ideal FD gas . Express your answer solely in terms of ñ ,, the mean number of particles in state r . ň , ( b ) Write a similar expression for the entropy S of a BE gas . ( c ) What do these expressions for S become in the classical ...
Contents
Introduction to statistical methods | 1 |
GENERAL DISCUSSION OF THE RANDOM WALK | 24 |
Statistical description of systems of particles | 47 |
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accessible amount approximation assume atoms becomes calculate called classical collision condition Consider consisting constant container corresponding course d³v defined denote depends derivatives described direction discussion distribution electrons energy ensemble entropy equal equation equilibrium evaluated example expression external field final follows force function given gives heat Hence ideal illustrated increase independent integral interaction interest internal involving liquid macroscopic magnetic mass maximum mean mean energy measured mechanics method molecules momentum Note obtains parameter particles particular partition phase physical position possible pressure probability problem properties quantity quantum quantum mechanics range relation relative remain reservoir respect result satisfy shows simply situation solid specific statistical steps sufficiently Suppose temperature theory thermal Thermodynamics tion unit variables velocity volume write written yields