Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 29
Frederick Reif. The ideal system of N spins has been described entirely in terms of quantum mechanics , but is otherwise completely analogous to the ideal gas of N molecules . In the case of the gas , each molecule moves about and ...
Frederick Reif. The ideal system of N spins has been described entirely in terms of quantum mechanics , but is otherwise completely analogous to the ideal gas of N molecules . In the case of the gas , each molecule moves about and ...
Page 40
Frederick Reif. Gas p 18 P P Vacuum Mercury Manometer Fig . 1.33 A gas whose average pressure p is measured by means ... ideal gas . Pressure of an ideal gas When a gas is confined within a container , the many collisions of the gas ...
Frederick Reif. Gas p 18 P P Vacuum Mercury Manometer Fig . 1.33 A gas whose average pressure p is measured by means ... ideal gas . Pressure of an ideal gas When a gas is confined within a container , the many collisions of the gas ...
Page 182
... ideal , what is the mean pressure p of this gas if its absolute temperature is T ? 4.15 Pressure and energy density of an ideal gas Use the expressions derived in Secs . 4.7 and 4.8 for the mean pressure p and the mean energy E of a gas ...
... ideal , what is the mean pressure p of this gas if its absolute temperature is T ? 4.15 Pressure and energy density of an ideal gas Use the expressions derived in Secs . 4.7 and 4.8 for the mean pressure p and the mean energy E of a gas ...
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