Tangent linear hard sphere chains: Difference between revisions
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==References== | ==References== | ||
#[http://dx.doi.org/10.1063/1.1389095 Carlos Vega, Carl McBride, and Luis G. MacDowell "Liquid crystal phase formation for the linear tangent hard sphere model from Monte Carlo simulations", Journal of Chemical Physics '''115''' pp. 4203-4211 (2001)] | #[http://dx.doi.org/10.1063/1.1389095 Carlos Vega, Carl McBride, and Luis G. MacDowell "Liquid crystal phase formation for the linear tangent hard sphere model from Monte Carlo simulations", Journal of Chemical Physics '''115''' pp. 4203-4211 (2001)] | ||
#[http://dx.doi.org/10.1080/00268979500102391 Dave C. Williamson and George Jackson "Excluded volume for a pair of linear chains of tangent hard spheres with an arbitrary relative orientation", Molecular Physics '''86''' pp. 819-836 (1995)] | |||
[[category:models]] | [[category:models]] |
Revision as of 13:30, 31 January 2008
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This model consists of, as the name suggests, chains of varying monomer length (), placed tangentially in a linear configuration. Each monomer is a hard sphere model and each molecule is rigid. For smectic-A phase beomes stable. For the nematic phase becomes stable.
References
- Carlos Vega, Carl McBride, and Luis G. MacDowell "Liquid crystal phase formation for the linear tangent hard sphere model from Monte Carlo simulations", Journal of Chemical Physics 115 pp. 4203-4211 (2001)
- Dave C. Williamson and George Jackson "Excluded volume for a pair of linear chains of tangent hard spheres with an arbitrary relative orientation", Molecular Physics 86 pp. 819-836 (1995)