2000
DOI: 10.1021/ma991666k
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Twist Viscosity of a Side-Chain Liquid-Crystalline Polysiloxane Dissolved in a Tumbling Nematic Solvent

Abstract: The dynamics of the twist distortion was characterized by electric-field-dependent dynamic light scattering (EFDLS) for a dilute solution of a side-chain liquid crystalline polysiloxane (SCLCP) dissolved in the tumbling nematic solvent, 4′-octyl-4-cyanobiphenyl (8CB). The results show a decrease in twist relaxation rate on dissolution of the SCLCP due to a large increase in twist viscosity δγ 1 with negligible change in twist elastic constant K22. By comparing the twist viscosity values, γ1 ) R3 -R2, with prev… Show more

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Cited by 6 publications
(6 citation statements)
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“…The anchoring energy is 9 ϫ 10 −6 J/m 2 for the linear line pattern with a pitch of 2.5 m. The bend and twist elastic constants used in the calculation are 4.9 ϫ 10 −12 and 2.4ϫ 10 −12 N, respectively. 24 This value is FIG. 3.…”
mentioning
confidence: 91%
“…The anchoring energy is 9 ϫ 10 −6 J/m 2 for the linear line pattern with a pitch of 2.5 m. The bend and twist elastic constants used in the calculation are 4.9 ϫ 10 −12 and 2.4ϫ 10 −12 N, respectively. 24 This value is FIG. 3.…”
mentioning
confidence: 91%
“…δγ 1 ∼ 0). 30,31 To rationalize these discrepancies, a phenomenological modification of the Brochard hydrodynamic model was proposed by Yao and Jamieson 15 which results in improved agreement with experiment. In particular, the theory enables a self-consistent treatment of ER data, stress transient data, and EFDLS results on solutions of a polysiloxane side-chain LCP in various LMMNs.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, the theory enables a self-consistent treatment of ER data, stress transient data, and EFDLS results on solutions of a polysiloxane side-chain LCP in various LMMNs. 15,[29][30][31] The modification is based on the assumption that for a LCP/LMMN solution an additional contribution to the hydrodynamic torque can arise from an elastic coupling between the LMMN director and the LCP director. 15 In the present work, we provide a further test of the hydrodynamic theory, using SANS measurements to directly probe the anisotropic radii of gyration R g| and R g⊥ of a side-chain polysiloxane LCP with cyanobiphenyl mesogenic side group dissolved in deuterated 4′-pentyl-4-cyanobiphenyl (5CB).…”
Section: Introductionmentioning
confidence: 99%
“…[11] There is also a tendency of the chain to be aligned with the field of the LMMN defining an anisotropic shape for the polymer. [12] The degree of anisotropy depends on the polymer backbone flexibility, molecular weight, spacer length, and if the polymer exhibits nematic or smectic phases. For the mixtures containing a liquid-crystalline polymer, the average nematic axis is defined by the director n of the LMMN; and although the polymer chains exhibit a distribution of orientations, the mesogenic groups in the polymer tend to orient parallel to the vector director of the liquid crystal solvent.…”
Section: Introductionmentioning
confidence: 99%
“…For the mixtures containing a liquid-crystalline polymer, the average nematic axis is defined by the director n of the LMMN; and although the polymer chains exhibit a distribution of orientations, the mesogenic groups in the polymer tend to orient parallel to the vector director of the liquid crystal solvent. [12] The aim of this work is to demonstrate the organization of microstructures formed by two different chiral side chain liquidcrystalline polymers (SCLCP), P 11M and P 4M , in 4 0 -n-pentyl-4-cyanobiphenyl (5CB) by means of polarized optical microscopy (POM). The POM technique allows a good understanding of the system, describing the mixtures according to the formed textures from the classic morphologies found in neat liquid crystals.…”
Section: Introductionmentioning
confidence: 99%