Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 74
... given molecule is found in the volume V , and q the probability that it is found in the remaining volume V ' . If the gas is in equilibrium , each mole- cule tends to be uniformly distributed throughout the box so that P = V Vo V ' and ...
... given molecule is found in the volume V , and q the probability that it is found in the remaining volume V ' . If the gas is in equilibrium , each mole- cule tends to be uniformly distributed throughout the box so that P = V Vo V ' and ...
Page 167
... given by the canonical distribution ( 49 ) or ( 51 ) ; i.e. , e - Ber P1 = Σεβετ where ẞ = 1 . kT ( 67 ) In ... given by Eq . ( 3.15 ) . Thus Er = π2h2 / n , 2 2m L12 n12 n22 + + L , 2 Lz 2 ( 68 ) The probability of finding the molecule ...
... given by the canonical distribution ( 49 ) or ( 51 ) ; i.e. , e - Ber P1 = Σεβετ where ẞ = 1 . kT ( 67 ) In ... given by Eq . ( 3.15 ) . Thus Er = π2h2 / n , 2 2m L12 n12 n22 + + L , 2 Lz 2 ( 68 ) The probability of finding the molecule ...
Page 183
... given by ( 3.13 ) . ( a ) Use this expression to calculate the force F , exerted by a photon on the right wall of the container when the photon is in a given state r specified by n , ny , n2 . 2 = ( b ) By simply averaging , derive an ...
... given by ( 3.13 ) . ( a ) Use this expression to calculate the force F , exerted by a photon on the right wall of the container when the photon is in a given state r specified by n , ny , n2 . 2 = ( b ) By simply averaging , derive an ...
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