Martynov Sarkisov Vompe: Difference between revisions

Revision as of 15:16, 20 June 2007

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

B^{(2)}(r)=-{\frac {1}{2}}(\omega -\phi )^{2}

where

\left.\phi \right.=\rho \epsilon \beta

where $\phi$ is short-ranged. The Weeks-Chandler-Anderson 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).

@@ Line 8: / Line 8: @@
 :<math>\left.\phi\right. =  \rho \epsilon \beta</math>
-where <math>\phi</math> is short-ranged. The [[WCA division]] of the [[Lennard-Jones model |Lennard-Jones]] potential was used.
+where <math>\phi</math> is short-ranged. The [[Weeks-Chandler-Anderson perturbation theory | Weeks-Chandler-Anderson division]] of the [[Lennard-Jones model |Lennard-Jones]] potential was used.
 (Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the [[Martynov Sarkisov]] closure).