Abstract

Liquid crystalline polymers have been extensively studied in shear starting from an equilibrium nematic phase. In this study, we explore the transient and long-time behavior as a steady shear cell experiment commences during an isotropic-nematic (I-N) phase transition. We initialize a localized Gaussian nematic droplet within an unstable isotropic phase with nematic, vorticity-aligned equilibrium at the walls. In the absence of flow, the simulation converges to a homogeneous nematic phase, but not before passing through quite intricate defect arrays and patterns due to physical anchoring, the dimensions of the shear cell, and transient backflow generated around the defect arrays during the I-N transition. Snapshots of this numerical experiment are then used as initial data for shear cell experiments at controlled shear rates. For homogeneous stable nematic equilibrium initial data, the Leal group [4, 5, 6] and the authors [12] confirm the Larson-Mead experimental observations [7, 8]: stationary 2-D roll cells and defect-free 2-D orientational structure at low shear rates, followed at higher shear rates by an unstable transition to an unsteady 2-D cellular flow and defect-laden attractor. We show at low shear rates that the memory of defect-laden data lasts forever; 2-D steady attractors of [4, 5, 12] emerge for defect free initial data, whereas 1-D unsteady attractors arise for defect-laden initial data.

Highlights

  • The Larson-Mead experiments on sheared nematic polymers [7, 8] identified roll cell formation at low shear rates, followed by roll cell instability

  • The sole purpose of the present paper is to explore what happens in these shear cell experiments if the initial data is non-homogeneous and defect-laden, with identical boundary conditions as previously reported

  • We choose data arising from an isotropic-nematic phase transition, which contains a complex mixture of isotropic and nematic domains, and for early times

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Summary

Introduction

The Larson-Mead experiments on sheared nematic polymers [7, 8] identified roll cell formation at low shear rates, followed by roll cell instability.

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