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驱动颗粒气体中的对称破缺不稳定性和强峰值周期聚集态

Symmetry-breaking instability and strongly peaked periodic clustering states in a driven granular gas.

作者信息

Livne Eli, Meerson Baruch, Sasorov Pavel V

机构信息

Racah Institute of Physics, Hebrew University of Jerusalem, Jerusalem 91904, Israel.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2002 Feb;65(2 Pt 1):021302. doi: 10.1103/PhysRevE.65.021302. Epub 2002 Jan 9.

Abstract

An ensemble of inelastically colliding grains driven by a horizontally vibrating wall in two dimensions exhibits clustering. Working in the limit of nearly elastic collisions and employing granular hydrodynamics, we predict, by a marginal stability analysis, a spontaneous symmetry breaking of the laterally uniform clustering state. Two-dimensional steady-state solutions found numerically describe laterally periodic clustering states. Well within the instability region the density of these states is strongly peaked, with most of the granulate located in "density islands." Time-dependent granular hydrodynamic simulations show that strongly peaked states can develop from small-amplitude single-mode density perturbations.

摘要

在二维空间中,由水平振动壁驱动的一组非弹性碰撞颗粒会出现聚集现象。在近弹性碰撞的极限情况下,并采用颗粒流体动力学,我们通过边际稳定性分析预测,横向均匀聚集态会发生自发对称性破缺。通过数值方法找到的二维稳态解描述了横向周期性聚集态。在不稳定性区域内,这些状态的密度强烈峰值化,大部分颗粒位于“密度岛”中。与时间相关的颗粒流体动力学模拟表明,强峰值状态可以从小振幅单模密度扰动发展而来。

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