Gibbs ensemble: Difference between revisions
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===Ergodic theory=== | ===[[Ergodic hypothesis |Ergodic theory]]=== | ||
Ref. 1 Eq. 2.6 | Ref. 1 Eq. 2.6 | ||
Revision as of 16:45, 21 November 2007
Here we have the N-particle distribution function (Ref. 1 Eq. 2.2)
where is a normalized constant with the dimensions of the phase space .
Normalization condition (Ref. 1 Eq. 2.3):
it is convenient to set (Ref. 1 Eq. 2.4)
where is the volume of the system and is the characteristic momentum of the particles (Ref. 1 Eq. 3.26),
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\mathcal {P}}={\sqrt {2\pi m\Theta }}}
Macroscopic mean values are given by (Ref. 1 Eq. 2.5)
Ergodic theory
Ref. 1 Eq. 2.6
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \langle \psi \rangle ={\overline {\psi }}}
Entropy
Ref. 1 Eq. 2.70
where Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \Omega } is the N-particle thermal potential (Ref. 1 Eq. 2.12)
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \Omega _{(N)}({\mathbf {X} }_{(N)},t)=\ln {\mathcal {G}}_{(N)}({\mathbf {X} }_{(N)},t)}
References
- G. A. Martynov "Fundamental Theory of Liquids. Method of Distribution Functions", Adam Hilger (out of print)