Nematic phase: Difference between revisions
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The response of a nematic liquid crystal | The response of a nematic liquid crystal | ||
to an external electric field depends on both the sign and the magnitude of <math>\Delta \epsilon</math>. | to an external electric field depends on both the sign and the magnitude of <math>\Delta \epsilon</math>. | ||
==Biaxial nematic phase== | |||
#[http://dx.doi.org/10.1016/j.fluid.2007.03.026 Carl McBride and Enrique Lomba "Hard biaxial ellipsoids revisited: Numerical results", Fluid Phase Equilibria '''255''' pp. 37-45 (2007)] | |||
#[http://dx.doi.org/10.1063/1.2815804 Roberto Berardi, Luca Muccioli, and Claudio Zannoni "Field response and switching times in biaxial nematics", Journal of Chemical Physics '''128''' 024905 (2008)] | |||
==References== | ==References== | ||
[[category: liquid crystals]] | [[category: liquid crystals]] |
Revision as of 11:07, 15 January 2008
The nematic phase has orientational order, but no positional order.
Discotic nematic phase
Dielectric tensor
In the uniaxial nematic phase, defining the z-axis to be parallel to the nematic axis, one has
The anisotropy is defined as
- .
The response of a nematic liquid crystal to an external electric field depends on both the sign and the magnitude of .
Biaxial nematic phase
- Carl McBride and Enrique Lomba "Hard biaxial ellipsoids revisited: Numerical results", Fluid Phase Equilibria 255 pp. 37-45 (2007)
- Roberto Berardi, Luca Muccioli, and Claudio Zannoni "Field response and switching times in biaxial nematics", Journal of Chemical Physics 128 024905 (2008)