Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 50
... discuss all such problems in the remainder of this book . Indeed , some of the questions which we have raised ( e.g. ... discussion will go a long way toward answering the most basic questions which we have raised . Summary of ...
... discuss all such problems in the remainder of this book . Indeed , some of the questions which we have raised ( e.g. ... discussion will go a long way toward answering the most basic questions which we have raised . Summary of ...
Page 151
... discussion shows that the tem- All the preceding measurements could be performed with any other thermometer M ' having a thermometric parameter 0 ' . There exists ordinarily a one - to - one relation between any value of 0 and the ...
... discussion shows that the tem- All the preceding measurements could be performed with any other thermometer M ' having a thermometric parameter 0 ' . There exists ordinarily a one - to - one relation between any value of 0 and the ...
Page 318
... discussion of such systems . In particular , it is not necessary to consider in detail the interactions which bring about the equilibrium situation ; it is quite sufficient to know that such interactions exist . But although equilibrium ...
... discussion of such systems . In particular , it is not necessary to consider in detail the interactions which bring about the equilibrium situation ; it is quite sufficient to know that such interactions exist . But although equilibrium ...
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