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 51
... phase space . The specification of the state of the system clearly becomes more precise as one decreases the size chosen for the cells into which phase space has been divided , i.e. , as one decreases the magnitude chosen for ho . Of ...
... phase space . The specification of the state of the system clearly becomes more precise as one decreases the size chosen for the cells into which phase space has been divided , i.e. , as one decreases the magnitude chosen for ho . Of ...
Page 51
... phase space . The specification of the state of the system clearly becomes more precise as one decreases the size chosen for the cells into which phase space has been divided , i.e. , as one decreases the magnitude chosen for ho . Of ...
... phase space . The specification of the state of the system clearly becomes more precise as one decreases the size chosen for the cells into which phase space has been divided , i.e. , as one decreases the magnitude chosen for ho . Of ...
Page 84
... phase space , draw separately the part of the phase space involving 1 and x , and that involving P1 and p2 . Indi- cate on these diagrams the regions of phase space accessible to the system . 2.3 Consider an ensemble of classical one ...
... phase space , draw separately the part of the phase space involving 1 and x , and that involving P1 and p2 . Indi- cate on these diagrams the regions of phase space accessible to the system . 2.3 Consider an ensemble of classical one ...
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