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	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_superball_model&amp;diff=20042</id>
		<title>Hard superball model</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_superball_model&amp;diff=20042"/>
		<updated>2018-04-02T21:56:55Z</updated>

		<summary type="html">&lt;p&gt;143.232.125.22: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:shape.png|thumb|right|The shape of superballs interpolates between octahedra (&#039;&#039;q&#039;&#039; = 0.5) and cubes (&#039;&#039;q&#039;&#039; = ∞) via spheres (&#039;&#039;q&#039;&#039; = 1).]]&lt;br /&gt;
[[Image:phase_diagram_superball.png|thumb|right|Phase diagram for hard superballs in the &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; (packing fraction) versus 1/&#039;&#039;q&#039;&#039; (bottom axis) and &#039;&#039;q&#039;&#039; (top axis) representation where &#039;&#039;q&#039;&#039; is the deformation parameter [2].]]&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;&#039;hard superball model&#039;&#039;&#039;  is defined by the inequality&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;|x|^{2q} + |y|^{2q} +|z|^{2q}  \le a^{2q}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039; and &#039;&#039;z&#039;&#039; are scaled Cartesian coordinates with &#039;&#039;q&#039;&#039; the deformation parameter and radius &#039;&#039;a&#039;&#039;. The shape of the superball interpolates smoothly between two Platonic solids, namely the octahedron (&#039;&#039;q&#039;&#039; = 0.5) and the [[Hard cube model |cube]] (&#039;&#039;q&#039;&#039; = ∞) via the [[Hard sphere model |sphere]] (&#039;&#039;q&#039;&#039; = 1) as shown in the right figure.&lt;br /&gt;
&lt;br /&gt;
== Particle Volume  == &lt;br /&gt;
The volume of a superball with the shape parameter &#039;&#039;q&#039;&#039; and radius &#039;&#039;a&#039;&#039; is given by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{align}&lt;br /&gt;
         v(q,a) &amp;amp; =  &amp;amp; 8 a^3 \int_{0}^1 \int_{0}^{(1-x^{2q})^{1/2q}} (1-x^{2q}-y^{2q})^{1/2q} \mathrm{d}\, y \, \mathrm{d}\, x = \frac{2a^3\left[ \Gamma\left(1/2q\right) \right]^3}{3q^2\Gamma\left(3/2q\right)},&lt;br /&gt;
\end{align}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt; is the [[Gamma function]].&lt;br /&gt;
&lt;br /&gt;
==Overlap algorithm==&lt;br /&gt;
The most widely used overlap algorithm is on the basis of Perram and Wertheim method &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0021-9991(85)90171-8  John W. Perram and M. S. Wertheim &amp;quot;Statistical mechanics of hard ellipsoids. I. Overlap algorithm and the contact function&amp;quot;, Journal of Computational Physics  &#039;&#039;&#039;58&#039;&#039;&#039; pp. 409-416 (1985)]&amp;lt;/ref&amp;gt; &amp;lt;ref name=&amp;quot;superballs&amp;quot;&amp;gt;[http://dx.doi.org/10.1039/C2SM25813G  R. Ni, A.P. Gantapara, J. de Graaf, R. van Roij, and M. Dijkstra &amp;quot;Phase diagram of colloidal hard superballs: from cubes via spheres to octahedra&amp;quot;, Soft Matter &#039;&#039;&#039;8&#039;&#039;&#039; pp. 8826-8834 (2012)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Phase diagram==&lt;br /&gt;
The full [[phase diagrams |phase diagram]] of hard superballs whose shape interpolates from cubes to octahedra was reported in Ref &amp;lt;ref name=&amp;quot;superballs&amp;quot;&amp;gt; &amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Models]]&lt;/div&gt;</summary>
		<author><name>143.232.125.22</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_superball_model&amp;diff=20041</id>
		<title>Hard superball model</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_superball_model&amp;diff=20041"/>
		<updated>2018-04-02T21:55:14Z</updated>

		<summary type="html">&lt;p&gt;143.232.125.22: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:shape.png|thumb|right|The shape of superballs interpolates between octahedra (&#039;&#039;q&#039;&#039; = 0.5) and cubes (&#039;&#039;q&#039;&#039; = ∞) via spheres (&#039;&#039;q&#039;&#039; = 1).]]&lt;br /&gt;
[[Image:phase_diagram_superball.png|thumb|right|Phase diagram for hard superballs in the &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; (packing fraction) versus 1/&#039;&#039;q&#039;&#039; (bottom axis) and &#039;&#039;q&#039;&#039; (top axis) representation where &#039;&#039;q&#039;&#039; is the deformation parameter [2].]]&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;&#039;hard superball model&#039;&#039;&#039;  is defined by the inequality&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;|x|^{2q} + |y|^{2q} +|z|^{2q}  \le a^{2q}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039; and &#039;&#039;z&#039;&#039; are scaled Cartesian coordinates with &#039;&#039;q&#039;&#039; the deformation parameter and radius &#039;&#039;a&#039;&#039;. The shape of the superball interpolates smoothly between two Platonic solids, namely the octahedron (&#039;&#039;q&#039;&#039; = 0.5) and the [[Hard cube model |cube]] (&#039;&#039;q&#039;&#039; = ∞) via the [[Hard sphere model |sphere]] (&#039;&#039;q&#039;&#039; = 1) as shown in the right figure.&lt;br /&gt;
&lt;br /&gt;
== Particle Volume  == &lt;br /&gt;
The volume of a superball with the shape parameter &#039;&#039;q&#039;&#039; and radius &#039;&#039;a&#039;&#039; is given by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{align}&lt;br /&gt;
         v(q,a) &amp;amp; =  &amp;amp; 8 a^3 \int_{0}^1 \int_{0}^{(1-x^{2q})^{1/2q}} (1-x^{2q}-y^{2q})^{1/2q} \mathrm{d}\, y \, \mathrm{d}\, x \\&lt;br /&gt;
         &amp;amp; = &amp;amp; \frac{2a^3\left[ \Gamma\left(1/2q\right) \right]^3}{3q^2\Gamma\left(3/2q\right)},&lt;br /&gt;
\end{align}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt; is the [[Gamma function]].&lt;br /&gt;
&lt;br /&gt;
==Overlap algorithm==&lt;br /&gt;
The most widely used overlap algorithm is on the basis of Perram and Wertheim method &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0021-9991(85)90171-8  John W. Perram and M. S. Wertheim &amp;quot;Statistical mechanics of hard ellipsoids. I. Overlap algorithm and the contact function&amp;quot;, Journal of Computational Physics  &#039;&#039;&#039;58&#039;&#039;&#039; pp. 409-416 (1985)]&amp;lt;/ref&amp;gt; &amp;lt;ref name=&amp;quot;superballs&amp;quot;&amp;gt;[http://dx.doi.org/10.1039/C2SM25813G  R. Ni, A.P. Gantapara, J. de Graaf, R. van Roij, and M. Dijkstra &amp;quot;Phase diagram of colloidal hard superballs: from cubes via spheres to octahedra&amp;quot;, Soft Matter &#039;&#039;&#039;8&#039;&#039;&#039; pp. 8826-8834 (2012)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Phase diagram==&lt;br /&gt;
The full [[phase diagrams |phase diagram]] of hard superballs whose shape interpolates from cubes to octahedra was reported in Ref &amp;lt;ref name=&amp;quot;superballs&amp;quot;&amp;gt; &amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Models]]&lt;/div&gt;</summary>
		<author><name>143.232.125.22</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_superball_model&amp;diff=20040</id>
		<title>Hard superball model</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_superball_model&amp;diff=20040"/>
		<updated>2018-04-02T21:53:55Z</updated>

		<summary type="html">&lt;p&gt;143.232.125.22: simplified definition of superball and volume formula&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:shape.png|thumb|right|The shape of superballs interpolates between octahedra (&#039;&#039;q&#039;&#039; = 0.5) and cubes (&#039;&#039;q&#039;&#039; = ∞) via spheres (&#039;&#039;q&#039;&#039; = 1).]]&lt;br /&gt;
[[Image:phase_diagram_superball.png|thumb|right|Phase diagram for hard superballs in the &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; (packing fraction) versus 1/&#039;&#039;q&#039;&#039; (bottom axis) and &#039;&#039;q&#039;&#039; (top axis) representation where &#039;&#039;q&#039;&#039; is the deformation parameter [2].]]&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;&#039;hard superball model&#039;&#039;&#039;  is defined by the inequality&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;|x|^{2q} + |y|^{2q} +|z|^{2q}  \le a^{2q}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039; and &#039;&#039;z&#039;&#039; are scaled Cartesian coordinates with &#039;&#039;q&#039;&#039; the deformation parameter and radius &#039;&#039;a&#039;&#039;. The shape of the superball interpolates smoothly between two Platonic solids, namely the octahedron (&#039;&#039;q&#039;&#039; = 0.5) and the [[Hard cube model |cube]] (&#039;&#039;q&#039;&#039; = ∞) via the [[Hard sphere model |sphere]] (&#039;&#039;q&#039;&#039; = 1) as shown in the right figure.&lt;br /&gt;
&lt;br /&gt;
== Particle Volume  == &lt;br /&gt;
The volume of a superball with the shape parameter &#039;&#039;q&#039;&#039; and radius &#039;&#039;a&#039;&#039; is given by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{align}&lt;br /&gt;
         v(q,a) &amp;amp; =  &amp;amp; 8 a^3 \int_{0}^1 \int_{0}^{(1-x^{2q})^{1/2q}} (1-x^{2q}-y^{2q})^{1/2q} \mathrm{d}\, y \, \mathrm{d}\, x \\&lt;br /&gt;
         &amp;amp; = &amp;amp; \frac{2a^3\left[ \Gamma\left(1+1/2q\right) \right]^3}{3q^2\Gamma\left(1+ 3/2q\right)},&lt;br /&gt;
\end{align}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt; is the [[Gamma function]].&lt;br /&gt;
&lt;br /&gt;
==Overlap algorithm==&lt;br /&gt;
The most widely used overlap algorithm is on the basis of Perram and Wertheim method &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0021-9991(85)90171-8  John W. Perram and M. S. Wertheim &amp;quot;Statistical mechanics of hard ellipsoids. I. Overlap algorithm and the contact function&amp;quot;, Journal of Computational Physics  &#039;&#039;&#039;58&#039;&#039;&#039; pp. 409-416 (1985)]&amp;lt;/ref&amp;gt; &amp;lt;ref name=&amp;quot;superballs&amp;quot;&amp;gt;[http://dx.doi.org/10.1039/C2SM25813G  R. Ni, A.P. Gantapara, J. de Graaf, R. van Roij, and M. Dijkstra &amp;quot;Phase diagram of colloidal hard superballs: from cubes via spheres to octahedra&amp;quot;, Soft Matter &#039;&#039;&#039;8&#039;&#039;&#039; pp. 8826-8834 (2012)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Phase diagram==&lt;br /&gt;
The full [[phase diagrams |phase diagram]] of hard superballs whose shape interpolates from cubes to octahedra was reported in Ref &amp;lt;ref name=&amp;quot;superballs&amp;quot;&amp;gt; &amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category: Models]]&lt;/div&gt;</summary>
		<author><name>143.232.125.22</name></author>
	</entry>
</feed>