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 118
... integral . this integral by the subscript " eq " ( standing for " equilibrium " ) to emphasize explicitly the fact that it is to be evaluated for any process by which the system is brought quasi - statically through a sequence of near ...
... integral . this integral by the subscript " eq " ( standing for " equilibrium " ) to emphasize explicitly the fact that it is to be evaluated for any process by which the system is brought quasi - statically through a sequence of near ...
Page 402
... integral eikz dx J ( k ) = √ _ 。( e2 + 1 ) ( e ̄2 + 1 ) 81 since power series expansion of J ( k ) yields the result ( 1 ) J ( k ) = ( ik ) m m ! Im ( 2 ) n = 0 = ( b ) Evaluate the integral J ( k ) by putting x = z , where z is a ...
... integral eikz dx J ( k ) = √ _ 。( e2 + 1 ) ( e ̄2 + 1 ) 81 since power series expansion of J ( k ) yields the result ( 1 ) J ( k ) = ( ik ) m m ! Im ( 2 ) n = 0 = ( b ) Evaluate the integral J ( k ) by putting x = z , where z is a ...
Page 609
... integral fe- dx cannot be evaluated in terms of elementary functions , although we have seen in Appendix A 2 that the definite integral between 0 and has the simple value √o " e ~ * dx = √F 2 ( A.5.1 ) Since the indefinite integral ...
... integral fe- dx cannot be evaluated in terms of elementary functions , although we have seen in Appendix A 2 that the definite integral between 0 and has the simple value √o " e ~ * dx = √F 2 ( A.5.1 ) Since the indefinite integral ...
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