Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
From inside the book
Results 1-3 of 38
Page 250
... heat reservoir at a temperature Thigh enough so that the oscillator can be described in terms of classical mechanics . Then the equipartition theorem ( 48 ) can be immediately applied to each of the quadratic ... Specific Heat of Solids.
... heat reservoir at a temperature Thigh enough so that the oscillator can be described in terms of classical mechanics . Then the equipartition theorem ( 48 ) can be immediately applied to each of the quadratic ... Specific Heat of Solids.
Page 262
... specific heat per mole of molecules thus adsorbed on a surface of fixed size ? 6.17 Temperature dependence of the electrical resistivity of a metal The electrical resistivity p of a metal is proportional to the probability that an ...
... specific heat per mole of molecules thus adsorbed on a surface of fixed size ? 6.17 Temperature dependence of the electrical resistivity of a metal The electrical resistivity p of a metal is proportional to the probability that an ...
Page 395
... specific heat , 248 specific heat at constant pressure , 309 velocity of sound , 281 monatomic , 167 nondegenerate , 166 , 176d polyatomic , 167 validity of classical discussion , 238-240 Gas constant , 174 numerical value , 195 , 381 ...
... specific heat , 248 specific heat at constant pressure , 309 velocity of sound , 281 monatomic , 167 nondegenerate , 166 , 176d polyatomic , 167 validity of classical discussion , 238-240 Gas constant , 174 numerical value , 195 , 381 ...
Contents
Characteristic Features of Macroscopic Systems | 1 |
Basic Probability Concepts | 55 |
Thermal Interaction | 141 |
Copyright | |
9 other sections not shown
Common terms and phrases
absolute temperature absorbed accessible approximation assume atoms average calculate classical collision Consider constant container cules definition denote discussion distribution electron ensemble entropy equal equilibrium situation equipartition theorem example expression external parameters fluctuations fluid function Gibbs free energy given heat capacity heat Q heat reservoir Hence ideal gas initial internal energy isolated system kinetic energy large number left half liquid macroscopic system macrostate magnetic field magnetic moment magnitude mass maximum mean energy mean number mean pressure mean value measured mole molecular momentum n₁ number of molecules occur oscillator particle particular phase phase space piston plane Poisson distribution position possible values Prob probability P(n quantity quantum numbers quasi-static random relation result simply solid specific heat statistical statistical ensemble statistically independent Suppose thermal contact thermally insulated thermometer tion total energy total number unit volume velocity