Transitions in Poiseuille flow of nematic liquid crystal

Recent experiments by Sengupta et al. (Phys. Rev. Lett. 2013) [9] revealed interesting transitions that can occur in flow of nematic liquid crystal under carefully controlled conditions within a long microfluidic channel of width much larger than height, and homeotropic anchoring at the walls. At lo...

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Veröffentlicht in:International journal of non-linear mechanics 2015-10, Vol.75 (C), p.15-21
Hauptverfasser: Anderson, T.G., Mema, E., Kondic, L., Cummings, L.J.
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Sprache:eng
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Zusammenfassung:Recent experiments by Sengupta et al. (Phys. Rev. Lett. 2013) [9] revealed interesting transitions that can occur in flow of nematic liquid crystal under carefully controlled conditions within a long microfluidic channel of width much larger than height, and homeotropic anchoring at the walls. At low flow rates the director field of the nematic adopts a configuration that is dominated by the surface anchoring, being nearly parallel to the channel height direction over most of the cross-section; but at high flow rates there is a transition to a flow-dominated state, where the director configuration at the channel centerline is aligned with the flow (perpendicular to the channel height direction). We analyze simple channel-flow solutions to the Leslie–Ericksen model for nematics. We demonstrate that two solutions exist, at all flow rates, but that there is a transition between the elastic free energies of these solutions: the anchoring-dominated solution has the lowest energy at low flow rates, and the flow-dominated solution has lowest energy at high flow rates. •We present a simple model, and exact solutions, for Poiseuille flow of nematic liquid crystal in a microfluidic.•We demonstrate the existence of two distinct solutions, and argue that these are analogous to two distinct states observed in experiments.•We propose an argument, based on energetics considerations, that explains the observed transitions between these two states.
ISSN:0020-7462
1878-5638
DOI:10.1016/j.ijnonlinmec.2015.04.010