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 139
Frederick Reif. 4.4 Heat capacity and specific heat Consider a macroscopic system whose macrostate can be specified by its absolute temperature T and some other ... of HEAT CAPACITY AND SPECIFIC HEAT 189 Heat capacity and specific heat.
Frederick Reif. 4.4 Heat capacity and specific heat Consider a macroscopic system whose macrostate can be specified by its absolute temperature T and some other ... of HEAT CAPACITY AND SPECIFIC HEAT 189 Heat capacity and specific heat.
Page 151
... heat capacity of this solid has an approximate temperature dependence given by Τ C ( T ) = - c ( 2-1 ) 1 if T1 < T < T1 = 0 otherwise The abrupt increase in specific heat as T is reduced below T1 is due to the onset of ferromagnetic ...
... heat capacity of this solid has an approximate temperature dependence given by Τ C ( T ) = - c ( 2-1 ) 1 if T1 < T < T1 = 0 otherwise The abrupt increase in specific heat as T is reduced below T1 is due to the onset of ferromagnetic ...
Page 392
... of these electrons is therefore unaffected by temperature so that these electrons contribute nothing to the heat capacity ( 9-16-12 ) . On the other hand , the small number Neff of electrons in the small energy range of order kT near ...
... of these electrons is therefore unaffected by temperature so that these electrons contribute nothing to the heat capacity ( 9-16-12 ) . On the other hand , the small number Neff of electrons in the small energy range of order kT near ...
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