# Difference between revisions of "Duh Haymet"

Carl McBride (talk | contribs) |
Carl McBride (talk | contribs) |
||

Line 4: | Line 4: | ||

:<math>B(\gamma^{*})= - \frac{1}{2} \gamma^{*2} \left[ \frac{1}{ \left[ 1+ \left( \frac{5\gamma^{*} +11}{7\gamma^{*} +9} \right) \gamma^{*} \right]} \right]</math> | :<math>B(\gamma^{*})= - \frac{1}{2} \gamma^{*2} \left[ \frac{1}{ \left[ 1+ \left( \frac{5\gamma^{*} +11}{7\gamma^{*} +9} \right) \gamma^{*} \right]} \right]</math> | ||

− | where (Eq. 10) <math>\gamma^{*}(r) = \gamma (r) - \beta \Phi_p(r)</math> where <math>\Phi_p (r)</math> is the perturbative (attractive) part of the pair potential. | + | where (Eq. 10) |

+ | |||

+ | :<math>\left. \gamma^{*}(r) \right.= \gamma (r) - \beta \Phi_p(r)</math> | ||

+ | |||

+ | where <math>\Phi_p (r)</math> is the perturbative (attractive) part of the [[Intermolecular pair potential | pair potential]]. | ||

## Revision as of 14:16, 7 June 2007

The **Duh-Haymet** (Ref. 1) (1995) Padé (3/2) approximation for the Bridge function for the Lennard-Jones system is (Eq. 13)

where (Eq. 10)

where is the perturbative (attractive) part of the pair potential.