Steady-state hydrodynamic instabilities of active liquid crystals: Hybrid lattice Boltzmann simulations

Details Steady-state hydrodynamic instabilities of active liquid crystals: Hybrid lattice Boltzmann simulations Steady-state hydrodynamic instabilities of active liquid crystals: Hybrid lattice Boltzmann simulations

2007-08-15

arxiv.org/abs/0708.2062v1

Physics

Condensed Matter

Soft Condensed Matter

18 eps figures, accepted for publication in Phys. Rev. E

Scientific paper

10.1103/PhysRevE.76.031921

We report hybrid lattice Boltzmann (HLB) simulations of the hydrodynamics of an active nematic liquid crystal sandwiched between confining walls with various anchoring conditions. We confirm the existence of a transition between a passive phase and an active phase, in which there is spontaneous flow in the steady state. This transition is attained for sufficiently ``extensile'' rods, in the case of flow-aligning liquid crystals, and for sufficiently ``contractile'' ones for flow-tumbling materials. In a quasi-1D geometry, deep in the active phase of flow-aligning materials, our simulations give evidence of hysteresis and history-dependent steady states, as well as of spontaneous banded flow. Flow-tumbling materials, in contrast, re-arrange themselves so that only the two boundary layers flow in steady state. Two-dimensional simulations, with periodic boundary conditions, show additional instabilities, with the spontaneous flow appearing as patterns made up of ``convection rolls''. These results demonstrate a remarkable richness (including dependence on anchoring conditions) in the steady-state phase behaviour of active materials, even in the absence of external forcing; they have no counterpart for passive nematics. Our HLB methodology, which combines lattice Boltzmann for momentum transport with a finite difference scheme for the order parameter dynamics, offers a robust and efficient method for probing the complex hydrodynamic behaviour of active nematics.

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