Hard ellipsoid model: Difference between revisions
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The most widely used overlap algorithm is that of Perram and Wertheim: | The most widely used overlap algorithm is that of Perram and Wertheim: | ||
*[http://dx.doi.org/:10.1016/0021-9991(85)90171-8 John W. Perram and M. S. Wertheim "Statistical mechanics of hard ellipsoids. I. Overlap algorithm and the contact function", Journal of Computational Physics '''58''' pp. 409-416 (1985)] | *[http://dx.doi.org/:10.1016/0021-9991(85)90171-8 John W. Perram and M. S. Wertheim "Statistical mechanics of hard ellipsoids. I. Overlap algorithm and the contact function", Journal of Computational Physics '''58''' pp. 409-416 (1985)] | ||
==Geometric properties== | |||
The mean radius of curvature is given by (Ref. 2) | |||
:<math>R= \frac{a}{2} \left[ \sqrt{\frac{1+\epsilon_b}{1+\epsilon_c}} + \sqrt \epsilon_c \left\{ \frac{1}{\epsilon_c} F(\varphi , k_1) + E(\varphi,k_1) \right\}\right], | |||
</math> | |||
and the surface area is given by | |||
:<math>S= 2 \pi a^2 \left[ 1+ \sqrt {\epsilon_c(1+\epsilon_b)} \left\{ \frac{1}{\epsilon_c} F(\varphi , k_2) + E(\varphi,k_2)\right\} \right], | |||
</math> | |||
where <math>F(\varphi,k)</math> is an [[elliptic integral]] of the first kind and <math>E(\varphi,k)</math> is an elliptic integral of the second kind, | |||
with the amplitude being | |||
:<math>\varphi = \tan^{-1} (\sqrt \epsilon_c),</math> | |||
and the moduli | |||
:<math>k_1= \sqrt{\frac{\epsilon_c-\epsilon_b}{\epsilon_c}},</math> | |||
and | |||
:<math>k_2= \sqrt{\frac{\epsilon_b (1+\epsilon_c)}{\epsilon_c(1+\epsilon_b)}},</math> | |||
where the anisotropy parameters, <math>\epsilon_b</math> and <math>\epsilon_c</math>, are | |||
:<math>\epsilon_b = \left( \frac{b}{a} \right)^2 -1,</math> | |||
and | |||
:<math>\epsilon_c = \left( \frac{c}{a} \right)^2 -1.</math> | |||
The volume of the ellipsoid is given by the well known | |||
:<math>V = \frac{4 \pi}{3}abc.</math> | |||
==See also== | ==See also== | ||
*[[Hard ellipsoid equation of state]] | *[[Hard ellipsoid equation of state]] | ||
==References== | ==References== | ||
#[http://dx.doi.org/10.1016/j.fluid.2007.03.026 Carl McBride and Enrique Lomba "Hard biaxial ellipsoids revisited: Numerical results", Fluid Phase Equilibria '''255''' pp. 37-45 (2007)] | #[http://dx.doi.org/10.1016/j.fluid.2007.03.026 Carl McBride and Enrique Lomba "Hard biaxial ellipsoids revisited: Numerical results", Fluid Phase Equilibria '''255''' pp. 37-45 (2007)] | ||
#[http://dx.doi.org/10.1063/1.472110 G. S. Singh and B. Kumar "Geometry of hard ellipsoidal fluids and their virial coefficients", Journal of Chemical Physics '''105''' pp. 2429-2435 (1996)] | |||
[[Category: Models]] | [[Category: Models]] |
Revision as of 12:07, 29 June 2007
Interaction Potential
The general ellipsoid, also called a triaxial ellipsoid, is a quadratic surface which is given in Cartesian coordinates by
where , and define the lengths of the axis.
Overlap algorithm
The most widely used overlap algorithm is that of Perram and Wertheim:
Geometric properties
The mean radius of curvature is given by (Ref. 2)
and the surface area is given by
where is an elliptic integral of the first kind and is an elliptic integral of the second kind, with the amplitude being
and the moduli
and
where the anisotropy parameters, and , are
and
The volume of the ellipsoid is given by the well known