Lattice Boltzmann simulations of spontaneous flow in active liquid crystals: The role of boundary conditions

J NON-NEWTON FLUID 149:1-3 (2008) 56-62

Authors:

D Marenduzzo, E Orlandini, ME Cates, JM Yeomans

Abstract:

Active liquid crystals or active gels are soft materials which can be physically realised, e.g. by preparing a solution of cytoskeletal filaments interacting with molecular motors. We study the hydrodynamics of an active liquid crystal in a slab-like geometry with various boundary conditions, by solving numerically its equations of motion via lattice Boltzmann simulations. In all cases we find that active liquid crystals can sustain spontaneous flow in steady state contrarily to their passive counterparts, and in agreement with recent theoretical predictions. We further find that conflicting anchoring conditions at the boundaries lead to spontaneous flow for any non-zero value of the 'activity' parameter, while with unfrustrated anchoring at all boundaries spontaneous flow only occurs when the activity exceeds a critical threshold. We finally discuss the dynamic pathway leading to steady state in a few selected cases. (c) 2007 Elsevier B.V. All fights reserved.

Publisher's Note: Paired composite-fermion wave functions [Phys. Rev. B 77, 075319 (2008)]

Physical Review B American Physical Society (APS) 77:7 (2008) 079905

Authors:

G Möller, SH Simon

Local density of states of 1D Mott insulators and CDW states with a boundary

(2008)

Authors:

Dirk Schuricht, Fabian HL Essler, Akbar Jaefari, Eduardo Fradkin

Order parameter statistics in the critical quantum Ising chain

(2008)

Authors:

Austen Lamacraft, Paul Fendley

Mechanical response of a small swimmer driven by conformational transitions.

Phys Rev Lett 100:3 (2008) 038101

Authors:

Ramin Golestanian, Armand Ajdari

Abstract:

A conformation space kinetic model is constructed to drive the deformation cycle of a three-sphere swimmer to achieve propulsion at low Reynolds number. We analyze the effect of an external load on the performance of this kinetic swimmer and show that it depends sensitively on where the force is exerted, so that there is no general force-velocity relation. We discuss how the conformational cycle of such swimmers should be designed to increase their performance in resisting forces applied at specific points.