Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 77
... assumes its possible values m = -4 , -2 , 0 , 2 , 4. Thus one has , by definition , m = ΣΡ ' ( m ) m m = [ × ( -4 ) ... assume the values and U1 , U2 , .... Ua U1 , U2 , .. ϋβ , respectively . Let us denote by P , the probability that u ...
... assumes its possible values m = -4 , -2 , 0 , 2 , 4. Thus one has , by definition , m = ΣΡ ' ( m ) m m = [ × ( -4 ) ... assume the values and U1 , U2 , .... Ua U1 , U2 , .. ϋβ , respectively . Let us denote by P , the probability that u ...
Page 88
... assume any value in the domain between 0 and 27. In the gen- eral case u can assume any value in some domain a1 ≤ u ≤ a2 . ( This domain be infinite in extent , i.e. , a1 → may both . ) Probability statements can be made about such a ...
... assume any value in the domain between 0 and 27. In the gen- eral case u can assume any value in some domain a1 ≤ u ≤ a2 . ( This domain be infinite in extent , i.e. , a1 → may both . ) Probability statements can be made about such a ...
Page 186
Frederick Reif. cule . In a quantum - mechanical description , this energy can assume the discrete values E ; ħ2j ( j + 1 ) = 2A ( i ) where the quantum number j , which determines the magnitude of the angular momentum J , can assume the ...
Frederick Reif. cule . In a quantum - mechanical description , this energy can assume the discrete values E ; ħ2j ( j + 1 ) = 2A ( i ) where the quantum number j , which determines the magnitude of the angular momentum J , can assume the ...
Contents
Characteristic Features of Macroscopic Systems | 1 |
Basic Probability Concepts | 55 |
Thermal Interaction | 141 |
Copyright | |
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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