Shear-banding fluid(s) under time-dependent shear flows. Part I: Spatiotemporal dynamics

We report on the response of semidilute shear-banding wormlike micelles to time-dependent flow protocols such as step stress and shear startup. We use global rheology coupled with direct optical visualizations in the Taylor-Couette flow to provide a detailed 2D description of the spatiotemporal dynamics of the shear banding flow under imposed stress. We compare these dynamics to their extensively studied counterpart under an imposed shear rate. We show that, for a given asymptotic state, the onset of banding is delayed and the transients are longer when the stress is used as a control parameter. The way the banding structure is built up strongly depends on the control parameter. In the two cases, secondary flows develop on top of the shear-banding instability: after shear startup, the interface between bands is formed in the bulk of the system and migrates inward to its stationary position in the gap of the Taylor-Couette device, before being destabilized due to elastic instability; under creep flow, the interface between bands forms at the inner wall and becomes wavy while it is still migrating outward to its steady position, leading to permanent rearrangements of the flow structure until a steady state is reached, potentially explaining longer transients. We also outline the possible mechanical signature of the onset of shear banding in terms of shape of the bulk mechanical signals, which is the subject of Part II of this work [Briole et al., J. Rheol., 65, 1201-1217 (2021)]. (c) 2021 The Society of Rheology. https://doi.org/10.1122/8.0000303

Automated summary

In this study, the response of semidilute shear-banding wormlike micelles to time-dependent flow protocols was reported. It was shown that the onset of banding is delayed and transients are longer when stress is used as a control parameter, and the way the banding structure is built up strongly depends on the control parameter. Additionally, secondary flows develop on top of the shear-banding instability in both cases, leading to different dynamics in the flow structure.