Gay-Berne model: Difference between revisions
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The '''Gay-Berne''' model is used extensively in simulations of [[liquid crystals | liquid crystalline]] systems. The Gay-Berne model | The '''Gay-Berne''' model is used extensively in simulations of [[liquid crystals | liquid crystalline]] systems. The Gay-Berne model | ||
is an anistropic form of the [[Lennard-Jones model | Lennard-Jones 12:6 potential]]. | is an anistropic form of the [[Lennard-Jones model | Lennard-Jones 12:6 potential]]. |
Revision as of 11:44, 27 September 2007
The Gay-Berne model is used extensively in simulations of liquid crystalline systems. The Gay-Berne model is an anistropic form of the Lennard-Jones 12:6 potential.
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)
- 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)
- Enrique De Miguel "Reexamining the phase diagram of the Gay-Berne fluid", Molecular Physics 100 pp. 2449-2459 (2002)
- Julian T. Brown, Michael P. Allen, Elvira Martín del Río and Enrique de Miguel "Effects of elongation on the phase behavior of the Gay-Berne fluid", Physical Review E 57 pp. 6685 - 6699 (1998)