Cousins J R L, Wilson S K, Mottram N J, Wilkes D, Weegels L
Department of Mathematics and Statistics, University of Strathclyde, Livingstone Tower, 26 Richmond Street, Glasgow G1 1XH, United Kingdom.
Merck KGaA, Frankfurter Strasse 250, Darmstadt 64293, Germany.
Phys Rev E. 2020 Dec;102(6-1):062703. doi: 10.1103/PhysRevE.102.062703.
Motivated by the one-drop-filling (ODF) method for the industrial manufacturing of liquid crystal displays, we analyze the pressure-driven flow of a nematic in a channel with dissipative weak planar anchoring at the boundaries of the channel. We obtain quasisteady asymptotic solutions for the director angle and the velocity in the limit of small Leslie angle, in which case the key parameters are the Ericksen number and the anchoring strength parameter. In the limit of large Ericksen number, the solution for the director angle has narrow reorientational boundary layers and a narrow reorientational internal layer separated by two outer regions in which the director is aligned at the positive Leslie angle in the lower half of the channel and the negative Leslie angle in the upper half of the channel. On the other hand, in the limit of small Ericksen number, the solution for the director angle is dominated by splay elastic effects with viscous effects appearing at first order. As the Ericksen number varies, there is a continuous transition between these asymptotic behaviors, and in fact the two asymptotic solutions capture the behavior rather well for all values of the Ericksen number. The steady-state value of the director angle at the boundaries and the timescale of the evolution toward this steady-state value in the asymptotic limits of large and small Ericksen number are determined. In particular, using estimated parameter values for the ODF method, it is found that the boundary director rotation timescale is substantially shorter than the timescale of the ODF method, suggesting that there is sufficient time for significant transient flow-driven distortion of the nematic molecules at the substrates from their required orientation to occur.
受液晶显示器工业制造中的一滴填充(ODF)方法的启发,我们分析了向列相在通道中的压力驱动流动,该通道在通道边界处具有耗散性弱平面锚定。我们在小莱斯利角的极限情况下获得了指向矢角和速度的准稳态渐近解,在这种情况下,关键参数是埃里克森数和锚定强度参数。在大埃里克森数的极限情况下,指向矢角的解具有狭窄的重取向边界层和一个狭窄的重取向内层,由两个外部区域隔开,在通道下半部分指向矢以正莱斯利角排列,在通道上半部分指向矢以负莱斯利角排列。另一方面,在小埃里克森数的极限情况下,指向矢角的解主要由展曲弹性效应主导,粘性效应在一阶出现。随着埃里克森数的变化,这些渐近行为之间存在连续过渡,实际上,对于埃里克森数的所有值,这两个渐近解都能很好地捕捉其行为。确定了在大、小埃里克森数的渐近极限情况下,边界处指向矢角的稳态值以及向该稳态值演化的时间尺度。特别是,使用ODF方法的估计参数值发现,边界指向矢旋转时间尺度明显短于ODF方法的时间尺度,这表明有足够的时间让基板处的向列相分子从所需取向发生显著的瞬态流动驱动畸变。