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		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Gay-Berne_model&amp;diff=11992</id>
		<title>Gay-Berne model</title>
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		<updated>2011-11-22T16:03:36Z</updated>

		<summary type="html">&lt;p&gt;137.187.78.82: spelling change&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;Gay-Berne model&#039;&#039;&#039; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.441483  J. G. Gay and B. J. Berne &amp;quot;Modification of the overlap potential to mimic a linear site–site potential&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;74&#039;&#039;&#039; pp. 3316-3319  (1981)]&amp;lt;/ref&amp;gt; is used extensively in simulations of [[liquid crystals | liquid crystalline]] systems. The Gay-Berne model&lt;br /&gt;
is an anisotropic form of the [[Lennard-Jones model | Lennard-Jones 12:6 potential]].&lt;br /&gt;
:&amp;lt;math&amp;gt;U_{ij}^{\mathrm LJ/GB} =&lt;br /&gt;
4 \epsilon_0^{\mathrm LJ/GB}&lt;br /&gt;
[\epsilon^{\mathrm LJ/GB}]^{\mu}&lt;br /&gt;
( {\mathbf {\hat u}}_j , {\mathbf {\hat r}}_{ij} )&lt;br /&gt;
\times  \left[ \left(&lt;br /&gt;
\frac{\sigma_0^{\mathrm LJ/GB}&lt;br /&gt;
}&lt;br /&gt;
{&lt;br /&gt;
r_{ij} -&lt;br /&gt;
\sigma^{\mathrm LJ/GB}&lt;br /&gt;
({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} )&lt;br /&gt;
+ {\sigma_0}^{\mathrm LJ/GB}&lt;br /&gt;
}&lt;br /&gt;
\right)^{12}&lt;br /&gt;
-&lt;br /&gt;
\left(&lt;br /&gt;
\frac&lt;br /&gt;
{&lt;br /&gt;
\sigma_0^{\mathrm LJ/GB}&lt;br /&gt;
}&lt;br /&gt;
{&lt;br /&gt;
r_{ij} -&lt;br /&gt;
\sigma^{\mathrm LJ/GB}&lt;br /&gt;
({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} )&lt;br /&gt;
+ {\sigma_0}^{\mathrm LJ/GB}&lt;br /&gt;
}&lt;br /&gt;
\right)^{6}&lt;br /&gt;
\right],&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where, in the limit of one of the particles being spherical, gives:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sigma^{\mathrm LJ/GB} ({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} ) ={\sigma_0}{[1 - \chi \alpha^{-2}&lt;br /&gt;
{({\mathbf {\hat{r}}}_{ij} \cdot  {\mathbf {\hat{u}}}_j )}^{2}]}^{-1/2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\epsilon^{\mathrm LJ/GB}({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} ) ={\epsilon_0}{[1 - \chi\prime  \alpha\prime^{-2}&lt;br /&gt;
{({\mathbf {\hat{r}}}_{ij} \cdot  {\mathbf {\hat{u}}}_j )}^{2}]}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\chi}{\alpha^{2}}=\frac{l_{j}^{2}-d_{j}^{2}}{l_{j}^{2}+d_{i}^{2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\chi \prime }{\alpha \prime^{2}}=1- {\left(\frac{\epsilon_{ee}}{\epsilon_{ss}}\right)} ^{\frac{1}{\mu}}.&amp;lt;/math&amp;gt;&lt;br /&gt;
==Phase diagram==&lt;br /&gt;
:&#039;&#039;Main article: [[Phase diagram of the Gay-Berne model]]&#039;&#039;&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1016/0009-2614(95)00212-M R. Berardi, C. Fava and C. Zannoni &amp;quot;A generalized Gay-Berne intermolecular potential for biaxial particles&amp;quot;, Chemical Physics Letters &#039;&#039;&#039;236&#039;&#039;&#039; pp. 462-468 (1995)]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevE.54.559  Douglas J. Cleaver, Christopher M. Care, Michael P. Allen, and Maureen P. Neal &amp;quot;Extension and generalization of the Gay-Berne potential&amp;quot; Physical Review E &#039;&#039;&#039;54&#039;&#039;&#039; pp. 559-567 (1996)]&lt;br /&gt;
*[http://dx.doi.org/10.1016/S0009-2614(98)01090-2 Roberto Berardi, Carlo Fava, Claudio Zannoni &amp;quot;A Gay–Berne potential for dissimilar biaxial particles&amp;quot;,  Chemical Physics Letters &#039;&#039;&#039;297&#039;&#039;&#039; pp. 8-14 (1998)]&lt;br /&gt;
[[category:liquid crystals]]&lt;br /&gt;
[[category:models]]&lt;/div&gt;</summary>
		<author><name>137.187.78.82</name></author>
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