Hard-sphere limit of soft-sphere model for granular materials: Stiffness dependence of steady granular flow

TL;DR

This study explores how steady granular flows behave as particles become increasingly stiff, revealing different limiting behaviors for collisional and frictional flow regimes in the hard-sphere limit.

Contribution

It provides a detailed numerical analysis of the stiffness dependence in the hard-sphere limit, distinguishing behaviors between collisional and frictional granular flows.

Findings

Collision rate converges to a finite value in collisional flow.

Contact time fraction with other particles goes to zero in collisional flow.

In frictional flow, the collision rate diverges as particle stiffness increases.

Abstract

Dynamical behavior of steady granular flow is investigated numerically in the inelastic hard sphere limit of the soft sphere model. We find distinctively different limiting behaviors for the two flow regimes, i.e., the collisional flow and the frictional flow. In the collisional flow, the hard sphere limit is straightforward; the number of collisions per particle per unit time converges to a finite value and the total contact time fraction with other particles goes to zero. For the frictional flow, however, we demonstrate that the collision rate diverges as the power of the particle stiffness so that the time fraction of the multiple contacts remains finite even in the hard sphere limit although the contact time fraction for the binary collisions tends to zero.