Abstract

Compared to isotropic liquids, orientational order of nematic liquid crystals makes their rheological properties more involved, and thus requires fine control of the flow parameters to govern the orientational patterns. In microfluidic channels with perpendicular surface alignment, nematics discontinuously transition from perpendicular structure at low flow rates to flow-aligned structure at high flow rates. Here we show how precise tuning of the driving pressure can be used to stabilize and manipulate a previously unresearched topologically protected chiral intermediate state which arises before the homeotropic to flow-aligned transition. We characterize the mechanisms underlying the transition and construct a phenomenological model to describe the critical behaviour and the phase diagram of the observed chiral flow state, and evaluate the effect of a forced symmetry breaking by introduction of a chiral dopant. Finally, we induce transitions on demand through channel geometry, application of laser tweezers, and careful control of the flow rate.

Highlights

  • Compared to isotropic liquids, orientational order of nematic liquid crystals makes their rheological properties more involved, and requires fine control of the flow parameters to govern the orientational patterns

  • Nematic liquid crystals (NLCs)[22] are fluids with orientational order of their anisotropic building blocks, which affects their rheological behaviour when confined to thin planar cells or a network of channels

  • We study a NLC flowing in thin microfluidic channels with perpendicular surface anchoring of nematic molecules on the channel walls

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Summary

Introduction

Orientational order of nematic liquid crystals makes their rheological properties more involved, and requires fine control of the flow parameters to govern the orientational patterns. Chiral order can emerge in intrinsically achiral liquid crystals[41,42,43], which is typically due to exclusion of certain elastic deformation modes and of the confinement[44,45,46,47] It is of particular interest if such chiral instabilities occur out of equilibrium, i.e. due to interaction with flow, and how such chiral modes couple with previously observed structural transitions and textures in Poiseuille flows of nematics[48,49,50,51,52,53,54,55,56]. We present a minimal phenomenological Landau model that reproduces the simulated phase behaviour and discuss the general behaviour of flowing anisotropic liquids

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