Statistical Physics, Part 1 |
From inside the book
Results 1-3 of 86
Page 73
... tion . It should be remembered that rotation in general changes the distribu- tion of mass in the body , and so the moment of inertia and internal energy of the body are themselves in general functions of 2 ( or of M ) . They may be ...
... tion . It should be remembered that rotation in general changes the distribu- tion of mass in the body , and so the moment of inertia and internal energy of the body are themselves in general functions of 2 ( or of M ) . They may be ...
Page 168
... tion n of the wave vector lying in the solid - angle element do . We can use the concept of the temperature of the radiation in each small interval of frequency and direction , defined as the temperature for which the density e ( w , n ) ...
... tion n of the wave vector lying in the solid - angle element do . We can use the concept of the temperature of the radiation in each small interval of frequency and direction , defined as the temperature for which the density e ( w , n ) ...
Page 462
... tion of the corresponding solution . The number n , thus defined may be either greater or less than the actual total number n of solute particles . If n ̧ = = n − n > O , this means that the solute accumulates at a higher concentra- tion ...
... tion of the corresponding solution . The number n , thus defined may be either greater or less than the actual total number n of solute particles . If n ̧ = = n − n > O , this means that the solute accumulates at a higher concentra- tion ...
Contents
Preface to the second English edition | 7 |
THE FUNDAMENTAL PRINCIPLES OF STATISTICAL PHYSICS | 7 |
1 Statistical distributions | 7 |
Copyright | |
134 other sections not shown
Other editions - View all
Common terms and phrases
adiabatic process angular momentum atoms Boltzmann Bose Bravais lattice calculate chemical potential closed system co-ordinates coefficient components condition constant corresponding curve decreases defined degrees of freedom denote density depends derivative determined differentials distribution function electron energy levels entropy equal equation expansion expression external Fermi gas finite fluctuations formula free energy frequency gases Gibbs distribution given gives Hamiltonian Hence ideal gas integral interaction kinetic energy lattice liquid macroscopic body mass matrix maximum mean value molecules momenta motion normalisation number of particles obtain P₁ partition function phase space phonons pressure probability distribution PROBLEM properties quantum mechanics quasi-particles regarded relation respect result rotation solid solution solvent specific heat spectrum spin substance Substituting subsystem suffix superfluid symmetry thermodynamic potential thermodynamic quantities tion total number V₁ vapour variables vector velocity vibrations volume wave functions ӘР