The role of dilation and confining stresses in shear thickening of dense suspensions

TL;DR

This study investigates the mechanisms behind Discontinuous Shear Thickening in dense suspensions, highlighting the roles of frictional interactions, dilation, and confining stresses from surface tension or boundaries, challenging traditional viscous models.

Contribution

It introduces a new model emphasizing frictional stresses and dilation effects, linking shear thickening to confining stresses from surface tension or boundary stiffness.

Findings

Shear thickening involves frictional rather than viscous interactions.

Onset stress correlates with hydrostatic pressure from particle weight.

Dilation and surface tension define the upper stress boundary.

Abstract

Many densely packed suspensions and colloids exhibit a behavior known as Discontinuous Shear Thickening in which the shear stress jumps dramatically and reversibly as the shear rate is increased. We performed rheometry and video microscopy measurements on a variety of suspensions to determine the mechanism for this behavior. Shear profiles and normal stress measurements indicate that, in the shear thickening regime, stresses are transmitted through frictional rather than viscous interactions, and come to the surprising conclusion that the local constitutive relation between stress and shear rate is not necessarily shear thickening. If the suspended particles are heavy enough to settle we find the onset stress of shear thickening tau_min corresponds to a hydrostatic pressure from the weight of the particle packing where neighboring particles begin to shear relative to each other. Above tau_min, dilation is seen to cause particles to penetrate the liquid-air interface of the sheared sample. The upper stress boundary tau_max of the shear thickening regime is shown to roughly match the ratio of surface tension divided by a radius of curvature on the order of the particle size. These results suggest a new model in which the increased dissipation in the shear thickening regime comes from frictional stresses that emerge as dilation is frustrated by a confining stress from surface tension at the liquid-air interface. When instead the suspensions are confined by solid walls and have no liquid-air interface, we find tau_max is set by the stiffness of the most compliant boundary which frustrates dilation. This rheology can be described by a non-local constitutive relation in which the local relation between stress and shear rate is shear thinning, but where the stress increase comes from a normal stress term which depends on the global dilation.