Force networks and jamming in shear deformed sphere packings
arXiv:1705.10109 · doi:10.1103/PhysRevE.99.012123
Abstract
The formation of self-organised structures that resist shear deformation have been discussed in the context of shear jamming and thickening[1-3], with frictional forces playing a key role. However, shear induces geometric features necessary for jamming even in frictionless packings[4]. We analyse conditions for jamming in such assemblies by solving force and torque balance conditions for their contact geometry. We demonstrate, and validate with frictional simulations, that the isostatic condition for mean contact number Z = D + 1 (for spatial dimension D = 2, 3) holds at jamming for both finite and infinite friction, above the random loose packing density. We show that the shear jamming threshold satisfies the marginal stability condition recently proposed for jamming in frictionless systems[5]. We perform rigidity percolation analysis[6,7] for D = 2 and find that rigidity percolation precedes shear jamming, which however coincides with the percolation of over-constrained regions, leading to the identification of an intermediate phase analogous to that observed in covalent glasses[8].
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- Shear jamming, discontinuous shear thickening, and fragile states in dry granular materials under oscillatory shear
- Sponge-like rigid structures in frictional granular packings
- The jamming transition is a k-core percolation transition
- Stress-stress Correlations Reveal Force Chains in Gels
- Timescale divergence at the shear jamming transition
- Microscopic Reversibility and Emergent Elasticity in Ultrastable Granular Systems
- Comparison of Shear and Compression Jammed Packings of Frictional Disks
- Criticality and marginal stability of the shear jamming transition of frictionless soft spheres