TY - JOUR
T1 - Flow patterns and disclination-density measurements in sheared nematic liquid crystals i
T2 - Flow-aligning 5cb
AU - Mather, P. T.
AU - Pearson, D. S.
AU - Larson, R. G.
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 1996
Y1 - 1996
N2 - We report the first direct measurements of disclination density during shear flow of a nematic liquid crystal. Samples of 4,4'-n-pentylcyanobiphenyl, or 5CB, are initially aligned in the homeotropic configuration within a torsional shear cell using surface treatment with lecithin. For low shearing rates, the director rotates within the shearing plane, except near the axis of rotation where irregular time-dependent out-of-plane orientation patterns exist. Disclinations form above a threshold shear rate, with the first ‘thick’ and ‘thin’ disclinations appearing near the sample edge, rapidly multiplying, and subsequently filling the sample. We measure the steady-state disclination density, pA, the length of disclinations per unit projection area. The dimensionless disclination density, pAh, where h is the sample thickness, is found to depend on two dimensionless quantities: Er, the Erickson number, and (Formula Presented), the scaled radial position. In the limit of large (Formula Presented), the dependence of pA on r disappears and we find the empirical relation pAh ∝ Er0.63.
AB - We report the first direct measurements of disclination density during shear flow of a nematic liquid crystal. Samples of 4,4'-n-pentylcyanobiphenyl, or 5CB, are initially aligned in the homeotropic configuration within a torsional shear cell using surface treatment with lecithin. For low shearing rates, the director rotates within the shearing plane, except near the axis of rotation where irregular time-dependent out-of-plane orientation patterns exist. Disclinations form above a threshold shear rate, with the first ‘thick’ and ‘thin’ disclinations appearing near the sample edge, rapidly multiplying, and subsequently filling the sample. We measure the steady-state disclination density, pA, the length of disclinations per unit projection area. The dimensionless disclination density, pAh, where h is the sample thickness, is found to depend on two dimensionless quantities: Er, the Erickson number, and (Formula Presented), the scaled radial position. In the limit of large (Formula Presented), the dependence of pA on r disappears and we find the empirical relation pAh ∝ Er0.63.
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U2 - 10.1080/02678299608031139
DO - 10.1080/02678299608031139
M3 - Article
AN - SCOPUS:0000112309
SN - 0267-8292
VL - 20
SP - 527
EP - 538
JO - Liquid Crystals
JF - Liquid Crystals
IS - 5
ER -