Farkas Illés J, Kun Jeromos, Jin Yi, He Gaoqi, Xu Mingliang
MTA-ELTE Statistical and Biological Physics Research Group (Hungarian Academy of Sciences), Pázmány Péter sétány 1A, Budapest 1117, Hungary and Regional Knowledge Center, ELTE Faculty of Sciences, Irányi Dániel u. 4., Székesfehérvár 8000, Hungary.
Department of Biological Physics, Eötvös University, Pázmány Péter sétány 1A, Budapest 1117, Hungary.
Phys Rev E Stat Nonlin Soft Matter Phys. 2015 Jan;91(1):012807. doi: 10.1103/PhysRevE.91.012807. Epub 2015 Jan 9.
The cohesive collective motion (flocking, swarming) of autonomous agents is ubiquitously observed and exploited in both natural and man-made settings, thus, minimal models for its description are essential. In a model with continuous space and time we find that if two particles arrive symmetrically in a plane at a large angle, then (i) radial repulsion and (ii) linear self-propelling toward a fixed preferred speed are sufficient for them to depart at a smaller angle. For this local gain of momentum explicit velocity alignment is not necessary, nor are adhesion or attraction, inelasticity or anisotropy of the particles, or nonlinear drag. With many particles obeying these microscopic rules of motion we find that their spatial confinement to a square with periodic boundaries (which is an indirect form of attraction) leads to stable macroscopic ordering. As a function of the strength of added noise we see--at finite system sizes--a critical slowing down close to the order-disorder boundary and a discontinuous transition. After varying the density of particles at constant system size and varying the size of the system with constant particle density we predict that in the infinite system size (or density) limit the hysteresis loop disappears and the transition becomes continuous. We note that animals, humans, drones, etc., tend to move asynchronously and are often more responsive to motion than positions. Thus, for them velocity-based continuous models can provide higher precision than coordinate-based models. An additional characteristic and realistic feature of the model is that convergence to the ordered state is fastest at a finite density, which is in contrast to models applying (discontinuous) explicit velocity alignments and discretized time. To summarize, we find that the investigated model can provide a minimal description of flocking.
在自然和人造环境中,都普遍观察到并利用了自主主体的凝聚集体运动(聚集、蜂拥),因此,描述它的最小模型至关重要。在一个具有连续空间和时间的模型中,我们发现,如果两个粒子以大角度对称地到达一个平面,那么(i)径向排斥和(ii)朝着固定的优选速度线性自推进足以使它们以较小角度离开。对于这种局部动量增益,明确的速度对齐不是必需的,粒子的粘附或吸引、非弹性或各向异性,或非线性阻力也不是必需的。当许多粒子遵循这些微观运动规则时,我们发现它们在具有周期性边界的正方形中的空间限制(这是一种间接的吸引形式)会导致稳定的宏观有序。作为添加噪声强度的函数,我们看到——在有限系统规模下——接近有序-无序边界时会出现临界减速和不连续转变。在恒定系统规模下改变粒子密度并在恒定粒子密度下改变系统规模之后,我们预测在无限系统规模(或密度)极限下,滞后回线消失,转变变为连续。我们注意到,动物、人类、无人机等往往异步移动,并且通常对运动比位置更敏感。因此,对于它们来说,基于速度的连续模型可以提供比基于坐标的模型更高的精度。该模型的另一个特征和现实特性是,在有限密度下收敛到有序状态最快,这与应用(不连续)明确速度对齐和离散时间的模型形成对比。总之,我们发现所研究的模型可以提供对聚集的最小描述。