Hanke Timo, Weber Christoph A, Frey Erwin
Arnold Sommerfeld Center for Theoretical Physics and Center for NanoScience, Department of Physics, Ludwig-Maximilians-Universität München, Theresienstraße 37, D-80333 Munich, Germany.
Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Nov;88(5):052309. doi: 10.1103/PhysRevE.88.052309. Epub 2013 Nov 19.
Collective motion in actively propelled particle systems is triggered on the very local scale by nucleation of coherently moving units consisting of just a handful of particles. These units grow and merge over time, ending up in a long-range ordered, coherently moving state. So far, there exists no bottom-up understanding of how the microscopic dynamics and interactions between the constituents are related to the system's ordering instability. In this paper, we study a class of models for propelled colloids allowing an explicit treatment of the microscopic details of the collision process. Specifically, the model equations are Newtonian equations of motion with separate force terms for particles' driving, dissipation, and interaction forces. Focusing on dilute particle systems, we analyze the binary scattering behavior for these models and determine-based on the microscopic dynamics-the corresponding "collision rule," i.e., the mapping of precollisional velocities and impact parameter on postcollisional velocities. By studying binary scattering we also find that the considered models for active colloids share the same principle for parallel alignment: The first incoming particle (with respect to the center of collision) is aligned to the second particle as a result of the encounter. This behavior distinctively differs from alignment in nondriven dissipative gases. Moreover, the obtained collision rule lends itself as a starting point to apply kinetic theory for propelled particle systems in order to determine the phase boundary to a long-range ordered, coherently moving state. The microscopic origin of the collision rule offers the opportunity to quantitatively scrutinize the predictions of kinetic theory for propelled particle systems through direct comparison with multiparticle simulations. We identify local precursor correlations at the onset of collective motion to constitute the essential determinant for a qualitative and quantitative validity of kinetic theory. In conclusion, our "renormalized" approach clearly indicates that the framework of kinetic theory is flexible enough to accommodate the complex behavior of soft active colloids and allows a bottom-up understanding of how the microscopic dynamics of binary collisions relates to the system's behavior on large length and time scales.
在主动推进的粒子系统中,集体运动在非常局部的尺度上由仅由少数几个粒子组成的相干运动单元的成核引发。这些单元随着时间的推移生长并合并,最终形成长程有序、相干运动的状态。到目前为止,对于组成部分之间的微观动力学和相互作用如何与系统的有序不稳定性相关,还没有自下而上的理解。在本文中,我们研究了一类推进胶体的模型,该模型允许对碰撞过程的微观细节进行明确处理。具体而言,模型方程是牛顿运动方程,具有分别用于粒子驱动、耗散和相互作用力的力项。聚焦于稀粒子系统,我们分析了这些模型的二元散射行为,并基于微观动力学确定了相应的“碰撞规则”,即碰撞前速度和碰撞参数到碰撞后速度的映射。通过研究二元散射,我们还发现所考虑的活性胶体模型具有相同的平行排列原理:第一个入射粒子(相对于碰撞中心)由于相遇而与第二个粒子对齐。这种行为与非驱动耗散气体中的排列明显不同。此外,所获得的碰撞规则可作为应用推进粒子系统动力学理论的起点,以确定到长程有序、相干运动状态的相边界。碰撞规则的微观起源提供了通过与多粒子模拟直接比较来定量审查推进粒子系统动力学理论预测的机会。我们确定集体运动开始时的局部前驱相关性是动力学理论定性和定量有效性的基本决定因素。总之,我们的“重整化”方法清楚地表明,动力学理论框架足够灵活,能够适应软活性胶体的复杂行为,并允许自下而上地理解二元碰撞的微观动力学如何与系统在大长度和时间尺度上的行为相关。