Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 64
... relation becomes P1 + P2 + Pa + P1 = 1 2 ( 2 ) where P1 = N / N denotes the probability of occurrence of event r in accordance with the definition ( 1 ) . The relation ( 2 ) , which states merely that the sum of all possible ...
... relation becomes P1 + P2 + Pa + P1 = 1 2 ( 2 ) where P1 = N / N denotes the probability of occurrence of event r in accordance with the definition ( 1 ) . The relation ( 2 ) , which states merely that the sum of all possible ...
Page 184
... relation F = 1 a ln Z BƏLz ( i ) Here Z is defined by the relation ( ii ) of the preceding problem . ( b ) In the case of any isotropic system , the function Z does not depend on the individual dimensions Lr , Ly , and Ly , but is ...
... relation F = 1 a ln Z BƏLz ( i ) Here Z is defined by the relation ( ii ) of the preceding problem . ( b ) In the case of any isotropic system , the function Z does not depend on the individual dimensions Lr , Ly , and Ly , but is ...
Page 280
... relation ( 56 ) is to be contrasted with the relation applicable in a quasi - static process where the gas is not thermally insulated , but is Note that ( 54 ) also follows immediately from ( 50 ) if one makes use of the general result ...
... relation ( 56 ) is to be contrasted with the relation applicable in a quasi - static process where the gas is not thermally insulated , but is Note that ( 54 ) also follows immediately from ( 50 ) if one makes use of the general result ...
Contents
Characteristic Features of Macroscopic Systems | 1 |
Basic Probability Concepts | 55 |
Thermal Interaction | 141 |
Copyright | |
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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