Yang Yingzi, Marceau Vincent, Gompper Gerhard
Theoretical Soft Matter and Biophysics, Institut für Festkörperforschung, Forschungszentrum Jülich, D-52425 Jülich, Germany.
Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Sep;82(3 Pt 1):031904. doi: 10.1103/PhysRevE.82.031904. Epub 2010 Sep 15.
Systems of self-propelled particles are known for their tendency to aggregate and to display swarm behavior. We investigate two model systems: self-propelled rods interacting via volume exclusion and sinusoidally beating flagella embedded in a fluid with hydrodynamic interactions. In the flagella system, beating frequencies are gaussian distributed with a nonzero average. These systems are studied by brownian-dynamics simulations and by mesoscale hydrodynamics simulations, respectively. The clustering behavior is analyzed as the particle density and the environmental or internal noise are varied. By distinguishing three types of cluster-size probability density functions, we obtain a phase diagram of different swarm behaviors. The properties of clusters such as their configuration, lifetime, and average size are analyzed. We find that the swarm behavior of the two systems, characterized by several effective power laws, is very similar. However, a more careful analysis reveals several differences. Clusters of self-propelled rods form due to partially blocked forward motion and are therefore typically wedge shaped. At higher rod density and low noise, a giant mobile cluster appears, in which most rods are mostly oriented toward the center. In contrast, flagella become hydrodynamically synchronized and attract each other; their clusters are therefore more elongated. Furthermore, the lifetime of flagella clusters decays more quickly with cluster size than of rod clusters.
自驱动粒子系统以其聚集倾向和呈现群体行为而闻名。我们研究了两个模型系统:通过体积排除相互作用的自驱动杆,以及嵌入具有流体动力学相互作用的流体中的正弦摆动鞭毛。在鞭毛系统中,摆动频率呈高斯分布且具有非零平均值。这些系统分别通过布朗动力学模拟和中尺度流体动力学模拟进行研究。随着粒子密度以及环境噪声或内部噪声的变化,对聚类行为进行了分析。通过区分三种类型的簇大小概率密度函数,我们得到了不同群体行为的相图。分析了簇的性质,如它们的构型、寿命和平均大小。我们发现,这两个系统以若干有效幂律为特征的群体行为非常相似。然而,更仔细的分析揭示了一些差异。自驱动杆的簇是由于向前运动部分受阻而形成的,因此通常呈楔形。在较高的杆密度和低噪声条件下,会出现一个巨大的移动簇,其中大多数杆大多朝向中心定向。相比之下,鞭毛在流体动力学上变得同步并相互吸引;因此它们的簇更细长。此外,鞭毛簇的寿命随簇大小的衰减比杆簇更快。