Editing Duh Haymet
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The '''Duh-Haymet''' (Ref. 1) (1995) Padé (3/2) approximation for the | The '''Duh-Haymet''' (Ref. 1) (1995) Padé (3/2) approximation for the Bridge function for the [[Lennard Jones]] system is (Eq. 13) | ||
<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 part of the pair potential | |||
(Note: in the [[WCA separation]] for the [[Lennard Jones]] system, the `perturbative part' is the attractive part). | |||
==References== | ==References== | ||
#[ | #[JCP_1995_103_02625] | ||