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黏弹性和弹性活性物质:线性不稳定性和非线性动力学。

Viscoelastic and elastomeric active matter: Linear instability and nonlinear dynamics.

机构信息

Department of Physics, Durham University, South Road, Durham DH1 3LE, United Kingdom.

DAMTP, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom.

出版信息

Phys Rev E. 2016 Mar;93(3):032702. doi: 10.1103/PhysRevE.93.032702. Epub 2016 Mar 15.

DOI:10.1103/PhysRevE.93.032702
PMID:27078422
Abstract

We consider a continuum model of active viscoelastic matter, whereby an active nematic liquid crystal is coupled to a minimal model of polymer dynamics with a viscoelastic relaxation time τ(C). To explore the resulting interplay between active and polymeric dynamics, we first generalize a linear stability analysis (from earlier studies without polymer) to derive criteria for the onset of spontaneous heterogeneous flows (strain rate) and/or deformations (strain). We find two modes of instability. The first is a viscous mode, associated with strain rate perturbations. It dominates for relatively small values of τ(C) and is a simple generalization of the instability known previously without polymer. The second is an elastomeric mode, associated with strain perturbations, which dominates at large τ(C) and persists even as τ(C)→∞. We explore the dynamical states to which these instabilities lead by means of direct numerical simulations. These reveal oscillatory shear-banded states in one dimension and activity-driven turbulence in two dimensions even in the elastomeric limit τ(C)→∞. Adding polymer can also have calming effects, increasing the net throughput of spontaneous flow along a channel in a type of drag reduction. The effect of including strong antagonistic coupling between the nematic and polymer is examined numerically, revealing a rich array of spontaneously flowing states.

摘要

我们考虑了一种主动粘弹性物质的连续体模型,其中主动向列液晶与聚合物动力学的最小模型耦合,具有粘弹性松弛时间 τ(C)。为了探索主动和聚合物动力学之间的相互作用,我们首先推广了线性稳定性分析(来自早期没有聚合物的研究),以推导出自发非均匀流动(应变速率)和/或变形(应变)开始的准则。我们发现了两种失稳模式。第一种是粘性模式,与应变速率扰动有关。对于相对较小的 τ(C)值,它占主导地位,是先前没有聚合物的已知不稳定性的简单推广。第二种是弹性体模式,与应变扰动有关,在较大的 τ(C)时占主导地位,甚至在 τ(C)→∞时也存在。我们通过直接数值模拟探索这些不稳定性导致的动力学状态。这些揭示了一维的振荡剪切带状状态和二维的活性驱动湍流,即使在弹性体极限 τ(C)→∞时也是如此。添加聚合物也可以产生镇静作用,增加沿通道的自发流动的净吞吐量,从而减少阻力。数值研究了包括向列和聚合物之间强拮抗耦合的影响,揭示了一系列丰富的自发流动状态。

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