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具有流体动力学的吸引性活性粒子的聚集与相行为

Clustering and phase behaviour of attractive active particles with hydrodynamics.

作者信息

Navarro Ricard Matas, Fielding Suzanne M

机构信息

Department of Physics, University of Durham, Science Laboratories, South Road, DH1 3LE, Durham, UK.

出版信息

Soft Matter. 2015 Oct 14;11(38):7525-46. doi: 10.1039/c5sm01061f.

Abstract

We simulate clustering, phase separation and hexatic ordering in a monolayered suspension of active squirming disks subject to an attractive Lennard-Jones-like pairwise interaction potential, taking hydrodynamic interactions between the particles fully into account. By comparing the hydrodynamic case with counterpart simulations for passive and active Brownian particles, we elucidate the relative roles of self-propulsion, interparticle attraction, and hydrodynamic interactions in determining clustering and phase behaviour. Even in the presence of an attractive potential, we find that hydrodynamic interactions strongly suppress the motility induced phase separation that might a priori have been expected in a highly active suspension. Instead, we find only a weak tendency for the particles to form stringlike clusters in this regime. At lower activities we demonstrate phase behaviour that is broadly equivalent to that of the counterpart passive system at low temperatures, characterized by regimes of gas-liquid, gas-solid and liquid-solid phase coexistence. In this way, we suggest that a dimensionless quantity representing the level of activity relative to the strength of attraction plays the role of something like an effective non-equilibrium temperature, counterpart to the (dimensionless) true thermodynamic temperature in the passive system. However there are also some important differences from the equilibrium case, most notably with regards the degree of hexatic ordering, which we discuss carefully.

摘要

我们模拟了在具有类似 Lennard-Jones 吸引性成对相互作用势的单层活性蠕动圆盘悬浮液中的聚集、相分离和六方有序,充分考虑了颗粒之间的流体动力学相互作用。通过将流体动力学情况与被动和主动布朗粒子的对应模拟进行比较,我们阐明了自推进、粒子间吸引力和流体动力学相互作用在决定聚集和相行为中的相对作用。即使存在吸引势,我们发现流体动力学相互作用强烈抑制了在高活性悬浮液中可能先验预期的运动诱导相分离。相反,我们发现在这种情况下粒子仅有一种形成串状聚集体的微弱趋势。在较低活性下,我们展示了与低温下对应被动系统大致等效的相行为,其特征是气 - 液、气 - 固和液 - 固共存相区。通过这种方式,我们表明一个代表活性水平相对于吸引力强度的无量纲量起到了类似于有效非平衡温度的作用,类似于被动系统中的(无量纲)真实热力学温度。然而,与平衡情况也存在一些重要差异,最显著的是关于六方有序程度,我们对此进行了仔细讨论。

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