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

被引:11
作者
Briole, Alice [1 ]
Casanellas, Laura [2 ]
Fardin, Marc-Antoine [3 ]
Py, Charlotte [1 ]
Cardoso, Olivier [1 ]
Browaeys, Julien [1 ]
Lerouge, Sandra [1 ]
机构
[1] Univ Paris, Lab Mat & Syst Complexes, CNRS, UMR 7057, 10 Rue Alice Domon & Leonie Duquet, F-75013 Paris, France
[2] Univ Montpellier, Lab Charles Coulomb, CNRS, UMR 5221, Pl Eugene Bataillon, F-34095 Montpellier 5, France
[3] Univ Paris, Inst Jacques Monod, CNRS, UMR 7592, 15 Rue Helene Brion, F-75013 Paris, France
关键词
Wormlike micelles; Shear banding; Flow dynamics; Elastic instability; Rheology; WORMLIKE MICELLAR-SOLUTION; TAYLOR-COUETTE; ELASTIC INSTABILITY; NONLINEAR RHEOLOGY; STRESS; SURFACTANT; BIREFRINGENCE; STABILITY; BEHAVIOR; NMR;
D O I
10.1122/8.0000303
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
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
引用
收藏
页码:1187 / 1200
页数:14
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