Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 215
... quasi - statically , the mean pres- sure p ( and energy E ) of the gas will then change accordingly . Suppose that ... static process which can be described by a curve showing successive values of the volume V and cor- responding mean ...
... quasi - statically , the mean pres- sure p ( and energy E ) of the gas will then change accordingly . Suppose that ... static process which can be described by a curve showing successive values of the volume V and cor- responding mean ...
Page 279
... quasi - statically from the initial macrostate a specified by ( To . Vo ) to ... static processes leading from an initial macrostate a , specified by a ... quasi - statically ; then the temperature and pressure of the gas must change ...
... quasi - statically from the initial macrostate a specified by ( To . Vo ) to ... static processes leading from an initial macrostate a , specified by a ... quasi - statically ; then the temperature and pressure of the gas must change ...
Page 305
... quasi - static manner . Further- more ( 108 ) implies that any engine which operates between these two reservoirs in a quasi - static manner has the same efficiency ; i.e. , for any quasi - static engine , n = T - T ' T ( 109 ) ...
... quasi - static manner . Further- more ( 108 ) implies that any engine which operates between these two reservoirs in a quasi - static manner has the same efficiency ; i.e. , for any quasi - static engine , n = T - T ' T ( 109 ) ...
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