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Shear flow of assemblies of cohesive and non-cohesive granular materials

机译:内聚和非内聚颗粒材料组件的剪切流

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摘要

We have studied plane shear flow of nearly homogeneous assemblies of uniformly sized, spherical particles in periodic domains. Our focus has been on the effect of interparticle attractive forces on the flow behavior manifested by dense assemblies. As a model problem, the cohesion resulting from van der Waals force acting between particles is considered. Simulations were performed for different strengths of cohesion, shear rates, particle stiffnesses, particle volume fractions and coefficients of friction. From each simulation, the average normal and shear stresses and the average coordination number have been extracted. Not surprisingly, the regimes of flow reported by Campbell [C.S. Campbell, Granular Shear Flows at the Elastic Limit, J. Fluid Mech. 465 (2002) 261-29 1] for the case of cohesionless particles - namely, inertial, elastic-inertial and elastic-quasistatic regimes - persist when cohesion is included. The elastic-quasistatic regime was found to correspond with the coordination number decreasing with increasing shear rate, while in the inertial regime the coordination number increased with shear rate. A striking result observed in the simulations is that the influence of cohesion on stress becomes more pronounced with decreasing particle volume fraction. Furthermore, the window in the shear rate-particle volume fraction space over which the elastic-quasistatic regime is obtained was found to expand as the strength of cohesion was increased. When the particle volume fraction is so high that even a cohesionless system would be in the elastic-quasistatic regime, the addition of cohesion had minimal effect on the stresses. At lower particle volume fractions where a cohesionless assembly would have been in the inertial regime, we present a new scaling which permits collapse of all the data at various strengths of cohesion and shear rates into a single master curve for each particle volume fraction and coefficient of friction. The regimes of flow in this master curve are discussed and the scaling for the normal stress in elastic-quasistatic flow is identified. (c) 2006 Elsevier B.V. All rights reserved.
机译:我们研究了周期域中大小均一的球形颗粒的近乎均匀的组件的平面剪切流。我们的研究重点是颗粒间吸引力对致密组件所表现出的流动行为的影响。作为模型问题,考虑了由范德华力作用在颗粒之间而产生的内聚力。针对不同的内聚强度,剪切速率,颗粒刚度,颗粒体积分数和摩擦系数进行了仿真。从每个模拟中,提取了平均法向应力和剪应力以及平均配位数。毫不奇怪,坎贝尔[C.S.坎贝尔,弹性极限的颗粒剪切流,J。流体力学。 465(2002)261-29 1]对于无内聚粒子的情况-即惯性,弹性惯性和弹性-准静态状态-在包含内聚时仍然存在。发现弹性准静态状态与配位数随剪切速率的增加而减小,而在惯性状态中,配位数随剪切速率的增加而增加。在模拟中观察到的惊人结果是,随着颗粒体积分数的减小,内聚力对应力的影响变得更加明显。此外,发现随着内聚强度的增加,获得弹性准静态状态的剪切速率-颗粒体积分数空间中的窗口扩大。当颗粒体积分数很高时,即使无内聚体系也将处于弹性准静态状态,内聚的添加对应力的影响很小。在较低的颗粒体积分数下,本来可以在无惯性状态下进行无内聚的组装,我们提出了一种新的标度,它允许将各种内聚力和剪切速率强度下的所有数据分解为每个颗粒体积分数和系数的一条主曲线。摩擦。讨论了该主曲线中的流态,并确定了准弹性流中法向应力的比例。 (c)2006 Elsevier B.V.保留所有权利。

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