Song and Mason perturbation theory: Difference between revisions
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The '''Song and Mason perturbation theory''' makes use of the [[Weeks-Chandler- | {{Stub-general}} | ||
The '''Song and Mason perturbation theory''' <ref>[http://dx.doi.org/10.1063/1.457252 Yuhua Song and E. A. Mason "Statistical-mechanical theory of a new analytical equation of state", Journal of Chemical Physics '''91''' pp. 7840-7853 (1989)]</ref> makes use of the [[Weeks-Chandler-Andersen perturbation theory | Weeks-Chandler-Andersen division]] of the potential, along with the [[Carnahan-Starling equation of state]] for the | |||
[[hard sphere model]]. | [[hard sphere model]]. | ||
==References== | ==References== | ||
<references/> | |||
[[category: perturbation theory]] | [[category: perturbation theory]] | ||
Latest revision as of 12:41, 16 February 2012
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The Song and Mason perturbation theory [1] makes use of the Weeks-Chandler-Andersen division of the potential, along with the Carnahan-Starling equation of state for the hard sphere model.