Martynov Sarkisov Vompe: Difference between revisions

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m (New page: The Martynov-Sarkisov-Vompe (MSV) (1999) (Eq. 33 Ref. 1) closure is given in terms of the bridge function :<math>B^{(2)}(r) = - \frac{1}{2} (\omega - \phi)^2</math> where :<math>\left....)
 
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:<math>\left.\phi\right. =  \rho \epsilon \beta</math>
:<math>\left.\phi\right. =  \rho \epsilon \beta</math>


where <math>\phi</math> is short-ranged. The [[WCA division]] of the LJ potential was used.
where <math>\phi</math> is short-ranged. The [[WCA division]] of the [[Lennard-Jones]] potential was used.
(Notice that the MSV closure, for a hard sphere fluid, becomes the MS closure).
(Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the [[Martynov Sarkisov]] closure).


==References==
==References==
#[JCP_1999_110_03961]
#[JCP_1999_110_03961]

Revision as of 12:48, 23 February 2007

The Martynov-Sarkisov-Vompe (MSV) (1999) (Eq. 33 Ref. 1) closure is given in terms of the bridge function

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle B^{(2)}(r) = - \frac{1}{2} (\omega - \phi)^2}

where

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left.\phi\right. = \rho \epsilon \beta}

where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi} is short-ranged. The WCA division of the Lennard-Jones potential was used. (Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the Martynov Sarkisov closure).

References

  1. [JCP_1999_110_03961]