Penetrable sphere model: Difference between revisions
		
		
		
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| m (Added mention of sigma) | Carl McBride (talk | contribs)  m (Added a little) | ||
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| </math> | </math> | ||
| where <math>\Phi_{12}(r)</math> is the [[intermolecular pair potential]], <math>\epsilon</math> is the hight of the repulsive core,  <math>r</math> is the distance between site 1 and site 2  <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> and <math>\sigma</math> is the radius of the core. Note: an earlier, different, penetrable sphere model was proposed, but is now known as the [[Widom-Rowlinson model]]. This model can be seen as the limiting case of the   | where <math>\Phi_{12}(r)</math> is the [[intermolecular pair potential]], <math>\epsilon</math> is the hight of the repulsive core,  <math>r</math> is the distance between site 1 and site 2  <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> and <math>\sigma</math> is the radius of the core. Note: an earlier, different, penetrable sphere model was proposed, but is now known as the [[Widom-Rowlinson model]]. This model can be seen as the limiting case of the [[Gaussian overlap model]] where <math>n \rightarrow \infty</math>. In the limit <math>\epsilon \rightarrow \infty</math> one has the [[hard sphere model]]. | ||
| [[Gaussian overlap model]] where <math>n \rightarrow \infty</math>. | |||
| ==References== | ==References== | ||
| <references/> | <references/> | ||
| [[category: models]] | [[category: models]] | ||
Latest revision as of 11:28, 23 May 2017
The penetrable sphere model is given by [1]:
where is the intermolecular pair potential, is the hight of the repulsive core, is the distance between site 1 and site 2 and is the radius of the core. Note: an earlier, different, penetrable sphere model was proposed, but is now known as the Widom-Rowlinson model. This model can be seen as the limiting case of the Gaussian overlap model where . In the limit one has the hard sphere model.