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Simulation of Cohesive Forces in Rapid Granular Flow Using a Square-Well Potential

机译:使用方阱势模拟快速颗粒流中的内聚力

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Cohesive interparticle forces have a significant effect in many granular flow applications. Consequently, many discrete-particle simulations of rapid granular flow have incorporated cohesive forces. On the other hand, efforts to incorporate cohesive interparticle forces into continuum models of rapid granular flow are limited. Continuum models use constitutive relations that are developed using kinetic theory, which assumes that all particle interactions are binary and instantaneous. This assumption of instantaneous particle interactions is inconsistent with cohesive force models that are typically a continuous function of particle separation distance. The square-well potential provides a way to incorporate cohesive interparticle forces into the system while still maintaining instantaneous, binary particle interactions. In the present study, rapid granular flows with attractive inter-particle forces are investigated. In particular, cohesive forces are incorporated into hard-sphere (molecular dynamics) simulations via a square-well potential. For simple shear flows, an investigation of the input parameter space indicates that two distinct flow regimes are present. For relatively large cohesive forces, the formation of a large, single agglomerate is observed. For moderate cohesive forces, the sheared system is composed of mostly 2- particle, dynamic agglomerates that are fairly evenly distributed throughout the domain. Furthermore, the results for this latter regime indicate that cohesion attenuates the magnitude of the stress components at higher solids fractions (in the collisional regime) as compared to the non-cohesive case. At lower solids fractions (kinetic regime), however the presence of cohesive forces has little impact on the observed stress due to the relatively large spacing between particles.
机译:内聚颗粒间力在许多颗粒流动应用中具有重要作用。因此,许多快速颗粒流动的离散粒子模拟都结合了内聚力。另一方面,将内聚颗粒间作用力纳入快速颗粒流动的连续模型的工作受到限制。连续体模型使用本构关系,该本构关系是使用动力学理论开发的,该理论假设所有粒子相互作用都是二元的和瞬时的。瞬时粒子相互作用的这种假设与内聚力模型不一致,内聚力模型通常是粒子分离距离的连续函数。平方阱电势提供了一种将内聚粒子间力整合到系统中的方法,同时仍保持瞬时的二元粒子相互作用。在本研究中,研究了具有吸引力的粒子间作用力的快速颗粒流。特别是,内聚力通过平方阱电势并入硬球(分子动力学)模拟中。对于简单的剪切流,对输入参数空间的研究表明存在两种不同的流态。对于较大的内聚力,观察到形成大的单个附聚物。对于适度的内聚力,剪切系统主要由2个粒子组成的动态团聚体,这些团聚体在整个区域中分布相当均匀。此外,后一种状态的结果表明,与非内聚情况相比,内聚力会降低较高固含量(在碰撞状态下)的应力分量的大小。在较低的固含量(运动状态)下,由于颗粒之间的相对较大的间距,内聚力的存在对观察到的应力几乎没有影响。

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