Yukawa closure: Difference between revisions

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m (New page: The '''Yukawa''' closure for hard spheres is <math>g_{ij}(r) \equiv h_{ij}(r) +1=0 ~~~~~~~~ r < \sigma_{ij} = (\sigma_i + \sigma_j)/2</math> and <math>c_{ij}(r)= \sum_{n=1} \frac{K_{ij}...)
 
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The '''Yukawa''' closure for hard spheres is
The '''Yukawa''' [[Closure relations | closure relation]] for [[hard sphere model | hard sphere]]s is


<math>g_{ij}(r) \equiv h_{ij}(r) +1=0 ~~~~~~~~ r < \sigma_{ij} = (\sigma_i + \sigma_j)/2</math>
:<math>g_{ij}(r) \equiv h_{ij}(r) +1=0 ~~~~~~~~ r < \sigma_{ij} = (\sigma_i + \sigma_j)/2</math>


and
and


<math>c_{ij}(r)= \sum_{n=1} \frac{K_{ij}}{r}e^{-z_nr} ~~~~~~ \sigma_{ij} < r </math>
:<math>c_{ij}(r)= \sum_{n=1} \frac{K_{ij}}{r}e^{-z_nr} ~~~~~~ \sigma_{ij} < r </math>
 
==References==
[[Category:Integral equations]]

Latest revision as of 19:16, 26 June 2007

The Yukawa closure relation for hard spheres is

and

References[edit]