Abstract
| Language | English |
|---|---|
| Pages | 281-295 |
| Number of pages | 14 |
| Journal | Continuum Mechanics and Thermodynamics |
| Volume | 14 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - Jun 2002 |
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Keywords
- molecular order
- director structure
- nematic liquid
- crystal cell
- magnetic field
- scalar order
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Magnetic field-induced changes in molecular order in nematic liquid crystals. / Mottram, N.J.; Hogan, S.J.
In: Continuum Mechanics and Thermodynamics, Vol. 14, No. 3, 06.2002, p. 281-295.Research output: Contribution to journal › Article
TY - JOUR
T1 - Magnetic field-induced changes in molecular order in nematic liquid crystals
AU - Mottram, N.J.
AU - Hogan, S.J.
PY - 2002/6
Y1 - 2002/6
N2 - We theoretically examine the effects of magnetic field-induced changes in molecular order and director structure within a nematic liquid crystal cell. As well as the cell thickness d there are two inherent characteristic lengths, the nematic correlation length z and the magnetic coherence length x. As the magnetic field increases the magnetic coherence length decreases and the relative ordering of the three length scales determines the director and scalar order parameter configuration through the cell. We use asymptotic expansions in regions defined by these length scales to analytically determine the molecular configuration in terms of these variables. Specifically, we investigate the boundary layer between the cell substrate and the bulk nematic material when strong anchoring forces the nematic director in a different direction to that of the applied field. We find that at low field strengths the classical picture of liquid crystal/magnetic field interaction occurs, that is, the director orientation is governed by the surface alignment until a transition occurs as the magnetic coherence length becomes comparable to the cell thickness and the director changes orientation so as to align with the magnetic field. At high field strengths, we find that a field-induced reduction of the molecular order occurs in a region close to the cell boundary. We are able to analytically determine the director and scalar order parameter configurations for the majority of field strengths and where analytical solutions are not found a numerical solution is presented. It is hoped that further work will extend this basis of analytical solutions to include a solution for all field strengths and for different cell configurations.
AB - We theoretically examine the effects of magnetic field-induced changes in molecular order and director structure within a nematic liquid crystal cell. As well as the cell thickness d there are two inherent characteristic lengths, the nematic correlation length z and the magnetic coherence length x. As the magnetic field increases the magnetic coherence length decreases and the relative ordering of the three length scales determines the director and scalar order parameter configuration through the cell. We use asymptotic expansions in regions defined by these length scales to analytically determine the molecular configuration in terms of these variables. Specifically, we investigate the boundary layer between the cell substrate and the bulk nematic material when strong anchoring forces the nematic director in a different direction to that of the applied field. We find that at low field strengths the classical picture of liquid crystal/magnetic field interaction occurs, that is, the director orientation is governed by the surface alignment until a transition occurs as the magnetic coherence length becomes comparable to the cell thickness and the director changes orientation so as to align with the magnetic field. At high field strengths, we find that a field-induced reduction of the molecular order occurs in a region close to the cell boundary. We are able to analytically determine the director and scalar order parameter configurations for the majority of field strengths and where analytical solutions are not found a numerical solution is presented. It is hoped that further work will extend this basis of analytical solutions to include a solution for all field strengths and for different cell configurations.
KW - molecular order
KW - director structure
KW - nematic liquid
KW - crystal cell
KW - magnetic field
KW - scalar order
UR - http://dx.doi.org/10.1007/s00161-002-0097-x
U2 - 10.1007/s00161-002-0097-x
DO - 10.1007/s00161-002-0097-x
M3 - Article
VL - 14
SP - 281
EP - 295
JO - Continuum Mechanics and Thermodynamics
T2 - Continuum Mechanics and Thermodynamics
JF - Continuum Mechanics and Thermodynamics
SN - 0935-1175
IS - 3
ER -