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In the study of [[liquid crystal]]s the '''paranematic susceptibility''' (Latin: susceptibilis “receptiveness”) is a quantity that describes the degree of induced order in a liquid crystal in response to an applied magnetic field. As a result of the diamagnetic anisotropy of liquid crystal molecules, nematic order can be produced by the application of a magnetic field. If a magnetic field is applied to a nematic liquid crystal in the isotropic phase then the order is given by: |
In the study of [[liquid crystal]]s the '''paranematic susceptibility''' (Latin: susceptibilis “receptiveness”) is a quantity that describes the degree of induced order in a liquid crystal in response to an applied magnetic field. As a result of the diamagnetic anisotropy of liquid crystal molecules, nematic order can be produced by the application of a magnetic field. If a magnetic field is applied to a nematic liquid crystal in the isotropic phase then the order is given by: |
Revision as of 06:24, 31 May 2020
This article needs more links to other articles to help integrate it into the encyclopedia. (September 2016) |
In the study of liquid crystals the paranematic susceptibility (Latin: susceptibilis “receptiveness”) is a quantity that describes the degree of induced order in a liquid crystal in response to an applied magnetic field. As a result of the diamagnetic anisotropy of liquid crystal molecules, nematic order can be produced by the application of a magnetic field. If a magnetic field is applied to a nematic liquid crystal in the isotropic phase then the order is given by:
The proportionality constant is the paranematic susceptibility. The value increases as the liquid crystal is cooled towards its transition temperature. In both the mean field approximation and Landau-deGennes theory the paranematic susceptibility is proportional to where is the transition temperature.
References
- E.B. Priestley, P.J. Wojtowicz, and P. Sheng, Introduction to Liquid Crystals, Plenum Press, 1974. ISBN 0-306-30858-4
- Sheng, Ping; Wojtowicz, Peter J. (1976-11-01). "Constant-coupling theory of nematic liquid crystals". Physical Review A. 14 (5). American Physical Society (APS): 1883–1894. doi:10.1103/physreva.14.1883. ISSN 0556-2791.