Pair stress approximation: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) (Added equation of state) |
Carl McBride (talk | contribs) mNo edit summary |
||
| Line 1: | Line 1: | ||
'''Pair stress approximation''' <ref>[http://dx.doi.org/10.1063/1.1669587 Emmanuel Meeron and Arnold J. F. Siegert "Statistical Mechanics of Hard‐Particle Systems", Journal of Chemical Physics '''48''' pp. 3139-3155 (1968)]</ref> (Eq. 3.18) | '''Pair stress approximation''' <ref>[http://dx.doi.org/10.1063/1.1669587 Emmanuel Meeron and Arnold J. F. Siegert "Statistical Mechanics of Hard‐Particle Systems", Journal of Chemical Physics '''48''' pp. 3139-3155 (1968)]</ref> for [[Idealised models#'Hard' models | hard particles]] is given by (Eq. 3.18) | ||
:<math>\rho B_2 = \frac{q}{(1+q)^{B_3}}</math> | :<math>\rho B_2 = \frac{q}{(1+q)^{B_3}}</math> | ||
Latest revision as of 15:35, 19 October 2011
Pair stress approximation [1] for hard particles is given by (Eq. 3.18)
where , is the second virial coefficient and is the third virial coefficient.
