1989
DOI: 10.1016/0167-2789(89)90104-8
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Pattern selection in nematics subjected to an elliptical shear

Abstract: Communicated by A.C. Newell We propose a simple nonlinear model to describe the onset of bimodal pattems in nematics (M.B.B.A. and T .N.C.) subjected to an elliptical shear. New expérimental resul ts which display the onset of secondary roUs before that of the bimodal pattems are al so presented and discussed.

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Cited by 5 publications
(2 citation statements)
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“…It is shown there that close to threshold the anisotropy favors a roll structure, and when f is increased the nonlinearity finally dominates resulting in destabilization of rolls and a transition to rectangles. A similar analysis was performed in the context of the elliptic shear instability in nematics based on a model amplitude equation [34]. Our work, however, provides the first stability analysis based The linear analysis of the oscillatory instability of RBC in a homeotropic nematic layer heated from below has been performed by several investigators [13, 25,35,36] and agreement [35] with the experiment [14] is rather good (see below).…”
Section: Barrattmentioning
confidence: 54%
“…It is shown there that close to threshold the anisotropy favors a roll structure, and when f is increased the nonlinearity finally dominates resulting in destabilization of rolls and a transition to rectangles. A similar analysis was performed in the context of the elliptic shear instability in nematics based on a model amplitude equation [34]. Our work, however, provides the first stability analysis based The linear analysis of the oscillatory instability of RBC in a homeotropic nematic layer heated from below has been performed by several investigators [13, 25,35,36] and agreement [35] with the experiment [14] is rather good (see below).…”
Section: Barrattmentioning
confidence: 54%
“…By another extension the rotational invariance is broken and describes some features of pattern formation in anisotropic systems, such as convection in planarly aligned nematic liquid crystals [17]. The interplay between a special form of the anisotropy and the broken up-down symmetry has been considered, too [18,19]. Here we generalize these models by combining the general anisotropic formulation with a quadratic nonlinearity: 0tu = (e (q( + V~) ju + bu~u~+ 2(a10( 020)0()u.…”
Section: Bothmentioning
confidence: 99%