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]]. | ||
<math>U_{ij}^{\mathrm LJ/GB} = | |||
4 \epsilon_0^{\mathrm LJ/GB} | |||
[\epsilon^{\mathrm LJ/GB}]^{\mu} | |||
( {\mathbf {\hat u}}_j , {\mathbf {\hat r}}_{ij} ) | |||
\times \left[ \left( | |||
\frac{\sigma_0^{\mathrm LJ/GB} | |||
} | |||
{ | |||
r_{ij} - | |||
\sigma^{\mathrm LJ/GB} | |||
({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} ) | |||
+ {\sigma_0}^{\mathrm LJ/GB} | |||
} | |||
\right)^{12} | |||
- | |||
\left( | |||
\frac | |||
{ | |||
\sigma_0^{\mathrm LJ/GB} | |||
} | |||
{ | |||
r_{ij} - | |||
\sigma^{\mathrm LJ/GB} | |||
({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} ) | |||
+ {\sigma_0}^{\mathrm LJ/GB} | |||
} | |||
\right)^{6} | |||
\right], | |||
</math> | |||
where, in the limit of one of the particles being spherical, gives: | |||
:<math>\sigma^{\mathrm LJ/GB} ({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} ) ={\sigma_0}{[1 - \chi \alpha^{-2} | |||
{({\mathbf {\hat{r}}}_{ij} \cdot {\mathbf {\hat{u}}}_j )}^{2}]}^{-1/2}</math> | |||
and | |||
:<math>\epsilon^{\mathrm LJ/GB}({\mathbf {\hat{u}}}_j, {\mathbf {\hat{r}}}_{ij} ) ={\epsilon_0}{[1 - \chi\prime \alpha\prime^{-2} | |||
{({\mathbf {\hat{r}}}_{ij} \cdot {\mathbf {\hat{u}}}_j )}^{2}]}</math> | |||
with | |||
:<math>\frac{\chi}{\alpha^{2}}=\frac{l_{j}^{2}-d_{j}^{2}}{l_{j}^{2}+d_{i}^{2}}</math> | |||
and | |||
:<math>\frac{\chi \prime }{\alpha \prime^{2}}=1- {\left(\frac{\epsilon_{ee}}{\epsilon_{ss}}\right)} ^{\frac{1}{\mu}}.</math> | |||
==References== | ==References== | ||
#[http://dx.doi.org/10.1063/1.441483 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)] | #[http://dx.doi.org/10.1063/1.441483 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)] |
Revision as of 11:04, 3 October 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. where, in the limit of one of the particles being spherical, gives:
and
with
and
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)