Abstract

Lyotropic chromonic liquid crystals (LCLCs) are a special type of hierarchical material in which self-assembled molecular aggregates are responsible for the formation of liquid crystal phases. Thanks to its unusual material properties and bio compatibility, it has found wide applications including the formation of active nematic liquid crystals. Recent experiments have uncovered tumbling character of certain LCLCs. However, how tumbling behavior modifies structure and flow in driven and active nematics is poorly understood. Here, we rely on continuum simulation to study the interplay of extensile active stress and externally driven flow in a flow-tumbling nematic with a low twist modulus to mimic nematic LCLCs. We find that a spontaneous transverse flow can be developed in a flow-tumbling active nematic confined to a hybrid alignment cell when it is in log-rolling mode at sufficiently high activities. The orientation of the total spontaneous flow is tunable by tuning the active stress. We further show that activity can suppress pressure-driven flow of a flow-tumbling nematic in a planar-anchoring cell but can also promote a transition of the director field under a pressure gradient in a homeotropic-anchoring cell. Remarkably, we demonstrate that the frequency of unsteady director dynamics in a tumbling nematic under Couette flow is invariant against active stress when below a threshold activity but exhibits a discontinuous increase when above the threshold at which a complex, periodic spatiotemporal director pattern emerges. Taken together, our simulations reveal qualitative differences between flow-tumbling and flow-aligning active nematics and suggest potential applications of tumbling nematics in microfluidics.

Highlights

  • Accepted: 31 August 2021Liquid crystal (LC) is a state of condensed matter intermediate between disordered liquid phase and highly ordered crystalline phase [1]

  • For a flow-tumbling nematic in the same hybrid cell, we find that a net flow along transverse direction can be developed in splay-bend tumbling nematic when the log-rolling mode appears at sufficiently high activity level

  • For a planar-anchoring cell, we find that pressure-driven flow can be enhanced and suppressed in flow-aligning and flow-tumbling nematic, respectively, due to the fact that the directors rotate in opposite handed directions for these two types of nematics

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Summary

Introduction

Accepted: 31 August 2021Liquid crystal (LC) is a state of condensed matter intermediate between disordered liquid phase and highly ordered crystalline phase [1]. A commonly studied LC phase is called the nematic phase in which anisotropic units, namely mesogens, of the LC develop long-range orientational ordering but remain spatially disordered [2]. Owing to the sensitivity of its orientational ordering relative to external stimuli and internal physicochemical events, nematic LCs have found wide applications in display, photonic devices and biosensing [3,4]. More recent applications of nematic LCs include directed self-assembly of colloids [5,6,7] and amphiphilic molecules [8,9]. In these applications, equilibrium structures and their thermodynamic stability at different conditions are concerned. There is a trend to understand and control transport and dynamics of nematic

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