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 80
Page 284
... expression ( 7 · 8.13 ) for μ , becomes identical to the simple expression ( 6-3-3 ) in the case where J = } . B 7.14 Consider an assembly of No weakly interacting magnetic atoms per unit volume at a temperature T and describe the ...
... expression ( 7 · 8.13 ) for μ , becomes identical to the simple expression ( 6-3-3 ) in the case where J = } . B 7.14 Consider an assembly of No weakly interacting magnetic atoms per unit volume at a temperature T and describe the ...
Page 538
... expression M = √ d3v Þ £ Þ - 2 f d3v Df ( 0 ) = f d3v ( £ Þ - 2 Df ( 0 ) ) ( 14-7-25 ) and the corresponding expression M ' calculated with the function ' , one finds by ( 14-7-23 ) and ( 14-7-24 ) that M'- M = 80 L 8P > 0 ( 14-7-26 ) ...
... expression M = √ d3v Þ £ Þ - 2 f d3v Df ( 0 ) = f d3v ( £ Þ - 2 Df ( 0 ) ) ( 14-7-25 ) and the corresponding expression M ' calculated with the function ' , one finds by ( 14-7-23 ) and ( 14-7-24 ) that M'- M = 80 L 8P > 0 ( 14-7-26 ) ...
Page 546
... expression for the electrical conductivity of the ions in this gas . 14.2 Consider again the physical situation described in Problem 13.6 where a mona- tomic dilute gas at temperature T is enclosed in a container and is maintained in ...
... expression for the electrical conductivity of the ions in this gas . 14.2 Consider again the physical situation described in Problem 13.6 where a mona- tomic dilute gas at temperature T is enclosed in a container and is maintained in ...
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 measured mechanics method mole 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