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		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_spherocylinders&amp;diff=10864</id>
		<title>Hard spherocylinders</title>
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		<summary type="html">&lt;p&gt;143.210.122.169: &lt;/p&gt;
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&lt;div&gt;[[Image:spherocylinder_purple.png|thumb|right]]&lt;br /&gt;
The &#039;&#039;&#039;hard spherocylinder&#039;&#039;&#039; model consists of an  impenetrable cylinder, capped at both ends &lt;br /&gt;
by hemispheres whose diameters are the same as the diameter of the cylinder. The hard spherocylinder model&lt;br /&gt;
has been studied extensively because of its propensity to form both [[Nematic phase | nematic]] and [[Smectic phases | smectic]] [[Liquid crystals | liquid crystalline]] phases. One of the first studies of  hard spherocylinders was undertaken by Cotter and Martire (Ref. 1) using [[scaled-particle theory]], and one of the first simulations was in the classic work of Jacques Vieillard-Baron  (Ref. 2). In the limit of zero diameter the hard spherocylinder becomes a line segment, often known as the [[3-dimensional hard rods |hard rod model]].&lt;br /&gt;
==Volume==&lt;br /&gt;
The molecular volume of the spherocylinder  is given by &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;v_0 = \pi \left( \frac{LD^2}{4} + \frac{D^3}{6} \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;L&amp;lt;/math&amp;gt; is the length of the cylindrical part of the spherocylinder and &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt; is the diameter.&lt;br /&gt;
==Minimum distance==&lt;br /&gt;
The minimum distance between two spherocylinders can be calculated using an algorithm published by Vega and Lago (Ref. 1). The [[Source code for the minimum distance between two rods | source code can be found here]]. Such an algorithm is essential in, for example, a [[Monte Carlo]] simulation, in order to check for overlaps between two sites.&lt;br /&gt;
#[http://dx.doi.org/10.1016/0097-8485(94)80023-5   Carlos Vega and Santiago Lago &amp;quot;A fast algorithm to evaluate the shortest distance between rods&amp;quot;, Computers &amp;amp; Chemistry  &#039;&#039;&#039;18&#039;&#039;&#039; pp. 55-59 (1994)]&lt;br /&gt;
==Virial coefficients==&lt;br /&gt;
:&#039;&#039;Main article: [[Hard spherocylinders: virial coefficients]]&#039;&#039;&lt;br /&gt;
==Phase diagram==&lt;br /&gt;
:&#039;&#039;Main aritcle: [[Phase diagram of the hard spherocylinder model]]&#039;&#039;&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Charged hard spherocylinders]]&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1063/1.1673232  Martha A. Cotter and Daniel E. Martire &amp;quot;Statistical Mechanics of Rodlike Particles. II. A Scaled Particle Investigation of the Aligned to Isotropic Transition in a Fluid of Rigid Spherocylinders&amp;quot;, Journal of Chemical Physics  &#039;&#039;&#039;52&#039;&#039;&#039; pp. 1909-1919 (1970)]&lt;br /&gt;
#[http://dx.doi.org/10.1080/00268977400102161 Jacques Vieillard-Baron  &amp;quot;The equation of state of a system of hard spherocylinders&amp;quot;, Molecular Physics &#039;&#039;&#039;28&#039;&#039;&#039; pp. 809-818 (1974)]&lt;br /&gt;
#[http://dx.doi.org/10.1021/j100303a008 Daan Frenkel &amp;quot;Onsager&#039;s spherocylinders revisited&amp;quot;, Journal of Physical Chemistry &#039;&#039;&#039;91&#039;&#039;&#039; pp. 4912-4916 (1987)]&lt;br /&gt;
#[http://dx.doi.org/10.1038/332822a0 D. Frenkel, H. N. W. Lekkerkerker and A. Stroobants &amp;quot;Thermodynamic stability of a smectic phase in a system of hard rods&amp;quot;, Nature &#039;&#039;&#039;332&#039;&#039;&#039; p. 822 (1988)]&lt;br /&gt;
[[Category: Models]]&lt;/div&gt;</summary>
		<author><name>143.210.122.169</name></author>
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