Shear thickening in suspensions of particles with dynamic brush layers

TL;DR

This study explores how dynamic covalent bonds between particles and polymers induce shear thickening in suspensions, revealing size-dependent onset stress and increased effective friction.

Contribution

It introduces a novel mechanism where molecular bridging creates controllable shear thickening, differing from traditional contact-based friction models.

Findings

Shear thickening onset stress scales with particle diameter as a power law with exponent -1.76.

Dynamic brush layers influence effective particle friction, increasing with decreasing particle size.

Enhanced dilation and reduced jamming volume fraction are observed in shear thickening regime.

Abstract

Control of frictional interactions among liquid-suspended particles has led to tunable, strikingly non-Newtonian rheology via the formation of strong flow constraints as particles come into close proximity under shear. Typically, these frictional interactions have been in the form of physical contact, controllable via particle shape and surface roughness. We investigate a different route, where molecular bridging between nearby particle surfaces generates a controllable "sticky" friction. This is achieved with surface-functionalized colloidal particles capable of forming dynamic covalent bonds with telechelic polymers that comprise the suspending fluid. At low shear stress this results in particles coated with a uniform polymer brush layer. Beyond an onset stress the telechelic polymers become capable of bridging and generate shear thickening. Over the size range investigated, we find that the dynamic brush layer leads to dependence of the onset stress on particle diameter that closely follows a power law with exponent -1.76. In the shear thickening regime, we observe an enhanced dilation in measurements of the first normal stress difference and reduction in the extrapolated volume fraction required for jamming, both consistent with an effective particle friction that increases with decreasing particle diameter. These results are discussed in light of predictions for suspensions of hard spheres and of polymer-grafted particles.