Shear shocks in fragile networks

TL;DR

This paper studies how shear waves propagate in fragile, disordered networks near a rigidity transition, revealing diffusive broadening, non-linear shear shocks, and energy cascades that differ from traditional elastic behavior.

Contribution

It introduces shear front rheology as an alternative to oscillatory rheology for analyzing fragile networks and uncovers the non-linear shock dynamics near the critical point.

Findings

Shear fronts exhibit diffusive broadening controlled by diverging shear viscosity.

Networks behave as over-damped due to energy leakage into non-affine fluctuations.

Non-linear shear shocks cause super-diffusive broadening and energy cascades.

Abstract

A minimal model for studying the mechanical properties of amorphous solids is a disordered network of point masses connected by unbreakable springs. At a critical value of its mean connectivity, such a network becomes fragile: it undergoes a rigidity transition signaled by a vanishing shear modulus and transverse sound speed. We investigate analytically and numerically the linear and non-linear visco-elastic response of these fragile solids by probing how shear fronts propagate through them. Our approach, that we tentatively label shear front rheology, provides an alternative route to standard oscillatory rheology. In the linear regime, we observe at late times a diffusive broadening of the fronts controlled by an effective shear viscosity that diverges at the critical point. No matter how small the microscopic coefficient of dissipation, strongly disordered networks behave as if they were over-damped because energy is irreversibly leaked into diverging non-affine fluctuations. Close to the transition, the regime of linear response becomes vanishingly small: the tiniest shear strains generate strongly non-linear shear shock waves qualitatively different from their compressional counterparts in granular media. The inherent non-linearities trigger an energy cascade from low to high frequency components that keep the network away from attaining the quasi-static limit. This mechanism, reminiscent of acoustic turbulence, causes a super-diffusive broadening of the shock width.