Duh Henderson: Difference between revisions

Latest revision as of 15:56, 22 May 2017

The Duh-Henderson bridge function ^[1] retains the Duh Haymet bridge function for $\gamma ^{*}\geq 0$ , and for $\gamma ^{*}\leq 0$ (Eq. 17):

B(\gamma ^{*})=-{\frac {1}{2}}\gamma ^{*2}

@@ Line 1: / Line 1: @@
-The '''Duh-Henderson'''  (Ref. 1) (1996) Bridge function
+The '''Duh-Henderson'''  [[bridge function]] <ref>[http://dx.doi.org/10.1063/1.471391      Der-Ming Duh and Douglas Henderson "Integral equation theory for Lennard-Jones fluids: The bridge function and applications to pure fluids and mixtures", Journal of Chemical Physics, '''104''' pp. 6742-6754  (1996)]</ref>
-retains the [[Duh Haymet]] Bridge function for  <math>\gamma^{*} \geq 0</math>, and for  <math>\gamma^{*} \leq 0</math> (Eq. 17)
+retains the [[Duh Haymet]] bridge function for  <math>\gamma^{*} \geq 0</math>, and for  <math>\gamma^{*} \leq 0</math> (Eq. 17):
 :<math>B(\gamma^{*})= - \frac{1}{2} \gamma^{*2}</math>
 ==References==
-#[JCP_1996_104_06742]
+<references/>
+;Related reading
+*[http://dx.doi.org/10.1080/00268976.2017.1292011 J. Karl Johnson, Douglas Henderson, Stanislav Labík and Anatol Malijevský "A comparison of the correlation functions of the Lennard–Jones fluid for the first-order Duh–Haymet–Henderson closure with molecular simulations", Molecular Physics '''115''' pp. 1335-1342 (2017)]
+[[Category: Integral equations]]