Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 156
... Q. Hence ( 37 ) implies that ΙΔ aß | AB | = | 3B Q | < B . ( 38 ) Since T = ( kẞ ) -1 or In T = -ln ẞ - Ink , it ... heat Q absorbed by a system is small whenever ( 38 ) is valid , i.e. , whenever Q is sufficiently small so that the ...
... Q. Hence ( 37 ) implies that ΙΔ aß | AB | = | 3B Q | < B . ( 38 ) Since T = ( kẞ ) -1 or In T = -ln ẞ - Ink , it ... heat Q absorbed by a system is small whenever ( 38 ) is valid , i.e. , whenever Q is sufficiently small so that the ...
Page 314
... heat q from some heat reservoir A at the absolute temperature T , reject heat q ' to some heat reservoir A ' at the lower absolute temperature T ' , and perform useful work w = q- q ' in the process . The simplest such engine is one ...
... heat q from some heat reservoir A at the absolute temperature T , reject heat q ' to some heat reservoir A ' at the lower absolute temperature T ' , and perform useful work w = q- q ' in the process . The simplest such engine is one ...
Page 314
... heat q from some heat reservoir A at the absolute temperature T , reject heat q ' to some heat reservoir A ' at the lower absolute temperature T ' , and perform useful work w = 9- q ' in the process . The simplest such engine is one ...
... heat q from some heat reservoir A at the absolute temperature T , reject heat q ' to some heat reservoir A ' at the lower absolute temperature T ' , and perform useful work w = 9- q ' in the process . The simplest such engine is one ...
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