Bandi M M, Rivera M K, Krzakala F, Ecke R E
MPA-10, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Apr;87(4):042205. doi: 10.1103/PhysRevE.87.042205. Epub 2013 Apr 18.
The granular jamming transition is experimentally investigated in a two-dimensional system of frictional, bidispersed disks subject to quasistatic, uniaxial compression without vibrational disturbances (zero granular temperature). Three primary results are presented in this experimental study. First, using disks with different static friction coefficients (μ), we experimentally verify numerical results that predict jamming onset at progressively lower packing fractions with increasing friction. Second, we show that the first compression cycle measurably differs from subsequent cycles. The first cycle is fragile-a metastable configuration with simultaneous jammed and unjammed clusters-over a small packing fraction interval (φ(1)<φ<φ(2)) and exhibits simultaneous exponential rise in pressure and exponential decrease in disk displacements over the same packing fraction interval. This fragile behavior is explained through a percolation mechanism of stressed contacts where cluster growth exhibits spatial correlation with disk displacements and contributes to recent results emphasizing fragility in frictional jamming. Control experiments show that the fragile state results from the experimental incompatibility between the requirements for zero friction and zero granular temperature. Measurements with several disk materials of varying elastic moduli E and friction coefficients μ show that friction directly controls the start of the fragile state but indirectly controls the exponential pressure rise. Finally, under repetitive loading (compression) and unloading (decompression), we find the system exhibits pressure hysteresis, and the critical packing fraction φ(c) increases slowly with repetition number. This friction-induced hysteretic creep is interpreted as the granular pack's evolution from a metastable to an eventual structurally stable configuration. It is shown to depend on the quasistatic step size Δφ, which provides the only perturbative mechanism in the experimental protocol, and the friction coefficient μ, which acts to stabilize the pack.
在一个二维摩擦双分散圆盘系统中,对颗粒堵塞转变进行了实验研究,该系统受到准静态单轴压缩且无振动干扰(颗粒温度为零)。本实验研究给出了三个主要结果。首先,使用具有不同静摩擦系数(μ)的圆盘,我们通过实验验证了数值结果,即随着摩擦力增加,堵塞起始点的堆积分数逐渐降低。其次,我们表明第一个压缩循环与后续循环有明显差异。第一个循环是脆弱的——在一个小的堆积分数区间(φ(1)<φ<φ(2))内是一种同时存在堵塞和未堵塞团簇的亚稳态构型,并且在相同堆积分数区间内压力呈指数上升而圆盘位移呈指数下降。这种脆弱行为通过应力接触的渗流机制来解释,其中团簇生长与圆盘位移呈现空间相关性,这也有助于解释近期强调摩擦堵塞中脆弱性的结果。对照实验表明,脆弱状态是由零摩擦和零颗粒温度要求之间的实验不相容性导致的。对几种具有不同弹性模量E和摩擦系数μ的圆盘材料进行测量表明,摩擦力直接控制脆弱状态的起始,但间接控制压力的指数上升。最后,在重复加载(压缩)和卸载(减压)下,我们发现系统呈现压力滞后现象,并且临界堆积分数φ(c)随着重复次数缓慢增加。这种摩擦诱导的滞后蠕变被解释为颗粒堆积从亚稳态向最终结构稳定构型的演化。结果表明它取决于准静态步长Δφ,其提供了实验方案中唯一的微扰机制,以及起到稳定堆积作用的摩擦系数μ。