Menzel Andreas M
Max Planck Institute for Polymer Research, P.O. Box 3148, DE-55021 Mainz, Germany.
Phys Rev E Stat Nonlin Soft Matter Phys. 2012 Feb;85(2 Pt 1):021912. doi: 10.1103/PhysRevE.85.021912. Epub 2012 Feb 16.
In this study, we investigate the phenomenon of collective motion in binary mixtures of self-propelled particles. More precisely, we consider two particle species, each of which consisting of pointlike objects that propel with a velocity of constant magnitude. Within each species, the particles try to achieve polar alignment of their velocity vectors, whereas we analyze the cases of preferred polar, antiparallel, as well as perpendicular alignment between particles of different species. Our focus is on the effect that the interplay between the two species has on the threshold densities for the onset of collective motion and on the nature of the solutions above onset. For this purpose, we start from suitable Langevin equations in the particle picture, from which we derive mean field equations of the Fokker-Planck type and finally macroscopic continuum field equations. We perform particle simulations of the Langevin equations and linear stability analyses of the Fokker-Planck and macroscopic continuum equations, and we numerically solve the Fokker-Planck equations. Both spatially homogeneous and inhomogeneous solutions are investigated, where the latter correspond to stripelike flocks of collectively moving particles. In general, the interaction between the two species reduces the threshold density for the onset of collective motion of each species. However, this interaction also reduces the spatial organization in the stripelike flocks. The case that shows the most interesting behavior is the one of preferred perpendicular alignment between different species. There a competition between polar and truly nematic orientational ordering of the velocity vectors takes place within each particle species. Finally, depending on the alignment rule for particles of different species and within certain ranges of particle densities, identical and inverted spatial density profiles can be found for the two particle species. The system under investigation is confined to two spatial dimensions.
在本研究中,我们探究了自驱动粒子二元混合物中的集体运动现象。更确切地说,我们考虑两种粒子,每种粒子都由以恒定大小速度推进的点状物体组成。在每种粒子内部,粒子试图使其速度矢量达到极性排列,而我们分析不同种类粒子之间优先极性、反平行以及垂直排列的情况。我们关注的是两种粒子之间的相互作用对集体运动开始时的阈值密度以及开始后解的性质所产生的影响。为此,我们从粒子图像中的合适朗之万方程出发,从中推导出福克 - 普朗克型的平均场方程,最终得到宏观连续场方程。我们对朗之万方程进行粒子模拟,并对福克 - 普朗克方程和宏观连续方程进行线性稳定性分析,同时数值求解福克 - 普朗克方程。我们研究了空间均匀和不均匀的解,其中后者对应于集体运动粒子的条纹状群聚。一般来说,两种粒子之间的相互作用降低了每种粒子集体运动开始时的阈值密度。然而,这种相互作用也降低了条纹状群聚中的空间组织性。表现出最有趣行为的情况是不同种类粒子之间优先垂直排列的情况。在这种情况下,每种粒子内部速度矢量的极性和真正向列取向有序之间会发生竞争。最后,根据不同种类粒子的排列规则以及在一定的粒子密度范围内,可以发现两种粒子具有相同和相反的空间密度分布。所研究的系统局限于二维空间。