Martynov Sarkisov Vompe

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

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

where

$\varphi =\rho ϵ\beta$

where $\varphi$ 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]