Yukawa closure - Revision history

Carl McBride at 17:16, 26 June 2007

2007-06-26T17:16:46Z

← Older revision		Revision as of 19:16, 26 June 2007
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	The [[Yukawa]] [[Closure relations \| closure relation]] for [[hard sphere model \| hard sphere]]s 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>

Carl McBride at 17:15, 26 June 2007

2007-06-26T17:15:12Z

← Older revision		Revision as of 19:15, 26 June 2007
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	The [[Yukawa]] closure for [[hard sphere model \| hard sphere]]s 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>

Carl McBride: Yukawa moved to Yukawa closure

2007-05-25T15:29:52Z

Yukawa moved to Yukawa closure

← Older revision	Revision as of 17:29, 25 May 2007
(No difference)

Carl McBride at 13:22, 21 March 2007

2007-03-21T13:22:47Z

← Older revision		Revision as of 15:22, 21 March 2007
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	The [[Yukawa]] closure for [[hard sphere]]s is		The [[Yukawa]] closure 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>

Carl McBride at 13:36, 27 February 2007

2007-02-27T13:36:23Z

← Older revision		Revision as of 15:36, 27 February 2007
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	The ~~'''~~Yukawa~~'''~~ closure for [[hard sphere]]s is		The [[Yukawa]] closure for [[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>

Nice and Tidy at 11:06, 27 February 2007

2007-02-27T11:06:28Z

← Older revision		Revision as of 13:06, 27 February 2007
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	==References==		==References==
			[[Category:Integral equations]]

Carl McBride at 11:44, 23 February 2007

2007-02-23T11:44:34Z

← Older revision		Revision as of 13:44, 23 February 2007
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	The '''Yukawa''' closure for hard ~~spheres~~ is		The '''Yukawa''' closure for [[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==

Carl McBride: New page: The '''Yukawa''' closure for hard spheres is $g_{ij}(r) \equiv h_{ij}(r) +1=0 ~~~~~~~~ r < \sigma_{ij} = (\sigma_i + \sigma_j)/2$ and $c_{ij}(r)= \sum_{n=1} \frac{K_{ij}...$

2007-02-19T19:03:19Z

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}...

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}}{r}e^{-z_nr} ~~~~~~ \sigma_{ij} < r </math>