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Computer simulation of thermotropic liquid crystals

The simulation of thermotropic liquid crystals is probably one of the hottest topics amongst computer modellers of condensed matters. This interest is largely motivated by the widening of areas in which liquid crystals offer revolutionary alternatives to conventional materials, the most famous example being that of the new generation LC displays.

But what exactly is a liquid crystal? A liquid crystalline phase is a phase ...in which long-range orientational order persists but molecular centres of mass are (to some extent) disordered and translationally mobile [Allen and Tildesley 1987]. By opposition to lyotropic LC (those found in detergents), thermotropic LC can be formed solely by a variation in thermal energy and do not require any interaction with a solvent. The simplest LC phase is known as the nematic phase in which the molecules centre of mass are translationally disordered but their axis are distributed along a preferred direction called the director.

The first attempts to simulate the formation of such systems were undertaken in the early 70's. The molecules were then represented as hard spherocylinders or hard ellipsoids of revolution. Although some evidence of the formation of a metastable orientationally ordered liquid phase were obtained, those simulations suffered from serious limitations.

Since then, the models were continuously refined to overcome those limitations. The most noticeable improvement is the use of soft orientation-dependent potentials such as the Gay-Bern potential described by its characteristic shape parameter:

(Hard to reproduce maths omitted!)

Indeed, he use of such potentials allows to gain a better understanding of the mechanisms involved in the formation of nematic LC phases by introducing anisotropic repulsive and attractive dispersion forces. An extensive series of simulations [Frenkel and Mulder 1985] allowed to obtain a complete phase diagram for hard ellipsoids of different length-to-width ratio. Current simulations produce results much closer to experimental data. The project consists in carrying out simple isothermal-isobaric NPT Monte Carlo simulations of a system of 512 hard ellipsoids of length-to-width ratio a/b = 5 interacting by a Gay-Berne potential. Observables such as the pair distribution function, g(r), the translational rho(k) and orientational order parameters P_2 can be monitored throughout the simulation to identify the occurrence of a phase transition. The project will be organised as two different stages:

The benefits of this project are obvious and multiple: firstly, the student will receive a good introduction to state-of-the-art computer modelling techniques. Furthermore, he will have the opportunity to develop his programming skills with a particular emphasis on optimisation techniques. This project gives a very good overview of the type of work expected during a PhD and as such can prove to be an invaluable experience for would-be PhD students.

Expertise Required

A good knowledge of Fortran or C would be welcome.

Resources Required

Workstations cluster.

Resources Supplied

Library of subroutines (Fortran77) from the CCP5 consortium, all necessary references.

References

[Allen and Tildesley 1987] Allen, M.,P. and Tildesley, D.,J. 1987. Computer Simulations of Liquids, Oxford University press. [Frenkel and Mulder 1985] Frenkel, D. and Mulder, B.,M. 1985. The hard ellipsoid-of-revolution fluid. I. Monte Carlo Simulations, Mol.,Phys. 55 1171--1192.

Gerbrand van der Zouw worked on this project.

Compressed PostScript of the project's final report is available here (395 bytes) .

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