Gay-Berne model: Difference between revisions
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==Phase diagram== | ==Phase diagram== | ||
:''Main article: [[Phase diagram of the Gay-Berne model]]'' | :''Main article: [[Phase diagram of the Gay-Berne model]]'' | ||
==See also== | |||
*[[Soft-core Gay-Berne model]] | |||
==References== | ==References== | ||
<references/> | <references/> |
Revision as of 13:23, 1 December 2016
The Gay-Berne model [1] is used extensively in simulations of liquid crystalline systems. The Gay-Berne model is an anisotropic form of the Lennard-Jones 12:6 potential.
where, in the limit of one of the particles being spherical, gives:
and
with
and
A modification of the Gay-Berne potential has recently been proposed that is said to result in a 10-20% improvement in computational speed, as well as accuracy [2].
Phase diagram
- Main article: Phase diagram of the Gay-Berne model
See also
References
- ↑ J. G. Gay and B. J. Berne "Modification of the overlap potential to mimic a linear site–site potential", Journal of Chemical Physics 74 pp. 3316-3319 (1981)
- ↑ Rasmus A. X. Persson "Note: Modification of the Gay-Berne potential for improved accuracy and speed", Journal of Chemical Physics 136 226101 (2012)
Related reading
- R. Berardi, C. Fava and C. Zannoni "A generalized Gay-Berne intermolecular potential for biaxial particles", Chemical Physics Letters 236 pp. 462-468 (1995)
- Douglas J. Cleaver, Christopher M. Care, Michael P. Allen, and Maureen P. Neal "Extension and generalization of the Gay-Berne potential" Physical Review E 54 pp. 559-567 (1996)
- Roberto Berardi, Carlo Fava, Claudio Zannoni "A Gay–Berne potential for dissimilar biaxial particles", Chemical Physics Letters 297 pp. 8-14 (1998)