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Some bifurcation problems in cholesteric liquid crystal theory

Published online by Cambridge University Press:  20 January 2009

P. J. Barratt
Affiliation:
University of Strathclyde
C. Fraser
Affiliation:
Dundee College of Technology
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A liquid crystal is a transversely isotropic liquid consisting of large, relatively rigid, elongated molecules which align more or less parallel to their neighbours. Three distinct types of liquid crystal occur, namely nematic, cholesteric and smectic. In the absence of any external influences, nematics tend to orientate with their anisotropic axis uniformly aligned, whereas cholesterics prefer a characteristic helical configuration and smectics are more highly organised in layered structures. However, it is possible to influence the orientation of the anisotropic axis by a variety of external means. In particular, solid surfaces affect the alignment through the action of surface torques, while electromagnetic fields exert body torques which tend to align the anisotropic axis either parallel or perpendicular to the applied field. Detailed descriptions of the physical properties of liquid crystals may be found in the books by de Gennes [1] and Chandrasekhar [2] and the review by Stephen and Straley [3].

Type
Research Article
Copyright
Copyright © Edinburgh Mathematical Society 1983

References

REFERENCES

1.De Gennes, P. G., The Physics of Liquid Crystals (Clarendon Press, Oxford, 1974).Google Scholar
2.Chandrasekhar, S., Liquid Crystals (University Press, Cambridge, 1977).Google Scholar
3.Stephen, M. J. and Straley, J. P., Physics of liquid crystals, Rev. Mod. Phys. 46 (1974), 617704.CrossRefGoogle Scholar
4.Freedericksz, F. and Zvolina, V., The orientation of an anisotropic liquid, Trans. Faraday Soc. 29 (1933), 919930.CrossRefGoogle Scholar
5.Schadt, M. and Helfrich, W., Voltage-dependent optical activity of a twisted nematic liquid crystal, Appl. Phys. Lett. 18 (1971), 127128.CrossRefGoogle Scholar
6.Raynes, E. P., Optically active additives in twisted nematic devices, Revue de Phys. Appl. 10 (1975), 117120.CrossRefGoogle Scholar
7.Ericksen, J. L., Equilibrium theory of liquid crystals, Adv. Liquid Cryst. 2 (1976), 233298.CrossRefGoogle Scholar
8.Leslie, F. M., Theory of flow phenomena in liquid crystals, Adv. Liquid Cryst. 4 (1979), 181.CrossRefGoogle Scholar
9.Deuling, H. J., Deformation of nematic liquid crystals in an electric field, Mol. Cryst. and Liquid Cryst. 19 (1972), 123131.CrossRefGoogle Scholar
10.Dafermos, C. M., Stability of orientation patterns of liquid crystals subject to magnetic fields, SIAM J. Appl. Maths. 16 (1968), 13051318.CrossRefGoogle Scholar
11.Leslie, F. M., Distortion of twisted orientation patterns in liquid crystals by magnetic fields, Mol. Cryst. and Liquid Cryst. 12 (1970), 5772.CrossRefGoogle Scholar
12.Nehring, J., Kmetz, A. R. and Scheffer, T. J., Analysis of weak-boundary-coupling effects in liquid crystal displays, J. Appl. Phys. 47 (1976), 850857.CrossRefGoogle Scholar
13.Straughan, B., Stability of uniform equilibrium states of a nematic liquid crystal, J. de Mecanique 19 (1980), 629638.Google Scholar