Gay-Berne model: Difference between revisions
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The '''Gay-Berne''' | The '''Gay-Berne model''' (Ref. 1) 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} = | :<math>U_{ij}^{\mathrm LJ/GB} = | ||
4 \epsilon_0^{\mathrm LJ/GB} | 4 \epsilon_0^{\mathrm LJ/GB} | ||
[\epsilon^{\mathrm LJ/GB}]^{\mu} | [\epsilon^{\mathrm LJ/GB}]^{\mu} | ||
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\right], | \right], | ||
</math> | </math> | ||
where, in the limit of one of the particles being spherical, gives: | where, in the limit of one of the particles being spherical, gives: | ||
Revision as of 10:11, 26 September 2008
The Gay-Berne model (Ref. 1) is used extensively in simulations of liquid crystalline systems. The Gay-Berne model is an anistropic form of the Lennard-Jones 12:6 potential.
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 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], }
where, in the limit of one of the particles being spherical, gives:
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \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}}
and
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \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}]}}
with
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{\chi}{\alpha^{2}}=\frac{l_{j}^{2}-d_{j}^{2}}{l_{j}^{2}+d_{i}^{2}}}
and
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{\chi \prime }{\alpha \prime^{2}}=1- {\left(\frac{\epsilon_{ee}}{\epsilon_{ss}}\right)} ^{\frac{1}{\mu}}.}
Phase diagram
- Main article: Phase diagram of the Gay-Berne model
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)