Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 48
... phase consists of the same kind of molecule ( H2O , in the case of water ) , but the molecules are arranged differently . In the gas phase , the molecules are far apart from each other and thus move about almost independently of each ...
... phase consists of the same kind of molecule ( H2O , in the case of water ) , but the molecules are arranged differently . In the gas phase , the molecules are far apart from each other and thus move about almost independently of each ...
Page 293
... phase 2 alone be present , or will both phases be present simultaneously ? Since the temperature T and pressure p ... phase 1 and G2 is that of phase 2 . But at a given temperature and pressure the mean energy , entropy , and volume of ...
... phase 2 alone be present , or will both phases be present simultaneously ? Since the temperature T and pressure p ... phase 1 and G2 is that of phase 2 . But at a given temperature and pressure the mean energy , entropy , and volume of ...
Page 294
... Phase 1 81 82 2 81 82 b Phase 2 T Fig . 7.10 A plot of pressure p versus tempera- ture T showing the regions where each of two phases exists separately in equilibrium and the phase - equilibrium curve where both phases can coexist in ...
... Phase 1 81 82 2 81 82 b Phase 2 T Fig . 7.10 A plot of pressure p versus tempera- ture T showing the regions where each of two phases exists separately in equilibrium and the phase - equilibrium curve where both phases can coexist in ...
Contents
Characteristic Features of Macroscopic Systems | 1 |
Basic Probability Concepts | 55 |
Thermal Interaction | 141 |
Copyright | |
9 other sections not shown
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