Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page xix
... Equipartition Theorem 246 6.6 Applications of the Equipartition Theorem 6.7 The Specific Heat of Solids 250 Summary of Definitions 256 Important Relations 256 Suggestions for Supplementary Reading 256 Problems 257 Chapter 7 General ...
... Equipartition Theorem 246 6.6 Applications of the Equipartition Theorem 6.7 The Specific Heat of Solids 250 Summary of Definitions 256 Important Relations 256 Suggestions for Supplementary Reading 256 Problems 257 Chapter 7 General ...
Page 223
... Equipartition Theorem 246 6.6 Applications of the Equipartition Theorem 6.7 The Specific Heat of Solids 250 Summary of Definitions 256 Important Relations 224 235 248 256 Suggestions for Supplementary Reading Problems 257 256 Chapter 6 ...
... Equipartition Theorem 246 6.6 Applications of the Equipartition Theorem 6.7 The Specific Heat of Solids 250 Summary of Definitions 256 Important Relations 224 235 248 256 Suggestions for Supplementary Reading Problems 257 256 Chapter 6 ...
Page 248
... gas . The agreement between the classical and quantum results is thus to be expected . Kinetic energy of a molecule in any gas Consider any 248 Canonical Distribution in the Classical Approximation Applications of the Equipartition Theorem.
... gas . The agreement between the classical and quantum results is thus to be expected . Kinetic energy of a molecule in any gas Consider any 248 Canonical Distribution in the Classical Approximation Applications of the Equipartition Theorem.
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