Martynov Vompe: Difference between revisions

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[[Lennard-Jones model | Lennard-Jones]] system, the `perturbative part' is the attractive part).
[[Lennard-Jones model | Lennard-Jones]] system, the `perturbative part' is the attractive part).
Martynov and Vompe have used the <math>dp_v-dP_c</math> and <math>dU-dP</math> [[thermodynamic consistencies]]
Martynov and Vompe have used the <math>dp_v-dP_c</math> and <math>dU-dP</math> [[thermodynamic consistencies]]
in constructing their closures <ref>#[http://dx.doi.org/10.1063/1.471522     Lloyd L. Lee, Dhananjay Ghonasgi, and Enrique Lomba "The fluid structures for soft-sphere potentials via the zero-separation theorems on molecular distribution functions", Journal of Chemical Physics '''104''' pp. 8058-8067  (1996)]</ref>.
in constructing their closures <ref>[http://dx.doi.org/10.1063/1.471522 Lloyd L. Lee, Dhananjay Ghonasgi, and Enrique Lomba "The fluid structures for soft-sphere potentials via the zero-separation theorems on molecular distribution functions", Journal of Chemical Physics '''104''' pp. 8058-8067  (1996)]</ref>.


==References==
==References==

Latest revision as of 12:43, 16 February 2012

The Martynov-Vompe closure relation [1] [2] is given by:

where

where is the perturbative part of the pair potential (Note: in the Weeks-Chandler-Andersen separation for the Lennard-Jones system, the `perturbative part' is the attractive part). Martynov and Vompe have used the and thermodynamic consistencies in constructing their closures [3].

References[edit]