Hard spherocylinders

The hard spherocylinder model consists on an impenetrable cylinder, capped at both ends by hemispheres whose diameters are the same as the diameter of the cylinder. The hard spherocylinder model has been studied extensively because of its propensity to form both nematic and smectic liquid crystalline phases. One of the first simulations of hard spherocylinders was in the classic work of Jacques Vieillard-Baron (Ref. 1).

Volume

The molecular volume of the spherocylinder is given by

$v_{0}=\pi \left({\frac {LD^{2}}{4}}+{\frac {D^{3}}{6}}\right)$

where $L$ is the length of the cylindrical part of the spherocylinder and $D$ is the diameter.

Minimum distance

The minimum distance between two spherocylinders can be calculated using an algorithm published by Vega and Lago (Ref. 1). The 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.

1. Carlos Vega and Santiago Lago "A fast algorithm to evaluate the shortest distance between rods", Computers & Chemistry 18 pp. 55-59 (1994)

Virial coefficients

Main article: Hard spherocylinders: virial coefficients

Phase diagram

Main aritcle: Phase diagram of the hard spherocylinder model

See also

• Charged hard spherocylinders

References

1. Jacques Vieillard-Baron "The equation of state of a system of hard spherocylinders", Molecular Physics 28 pp. 809-818 (1974)
2. Daan Frenkel "Onsager's spherocylinders revisited", Journal of Physical Chemistry 91 pp. 4912-4916 (1987)
3. D. Frenkel, H. N. W. Lekkerkerker and A. Stroobants "Thermodynamic stability of a smectic phase in a system of hard rods", Nature 332 p. 822 (1988)