Paper Number
IN8
Session
Flow Induced Instabilities and Non-Newtonian Fluids
Title
Interplay between shear banding and wall slip: Generalized lever rule
Presentation Date and Time
October 21, 2019 (Monday) 2:20
Track / Room
Track 4 / Room 305B
Authors
- Geri, Michela (MIT, Mechanical Engineering)
- Saint-Michel, Brice (Imperial College)
- Divoux, Thibaut (MIT,CNRS)
- Manneville, Sebastien (ENS Lyon)
- McKinley, Gareth H. (Massachusetts Institute of Technology, Department of Mechanical Engineering)
Author and Affiliation Lines
Michela Geri1, Brice Saint-Michel2, Thibaut Divoux3, Sebastien Manneville4, and Gareth H. McKinley1
1Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, MA; 2Imperial College, London, United Kingdom; 3MIT,CNRS, Cambridge, MA 02139; 4ENS Lyon, Lyon, France
Speaker / Presenter
Geri, Michela
Text of Abstract
Shear banding has been shown to affect the flow of many complex fluids under simple viscometric conditions. A common feature of steady-state shear banding is the presence of a non-monotonic branch in the underlying flow curve. In thixotropic yield stress fluids banding usually occurs when the applied shear-rate is smaller than a critical value and is characterized by an arrested band adjacent to a steady sheared region; the stress measured during flow is usually constant and equal to the apparent yield stress. In this work, we show that steady-state shear banding in a thixotropic yield stress fluid with inherently different thixotropic time scales (for the plastic viscosity and yield stress) allows us to partially measure the non-monotonic branch of the flow curve in a rheometer. The test fluid consists of a suspension of microscopic paraffin platelets in mineral oil at different concentrations. Rheometric tests under decreasing shear rates are performed in a bespoke Couette cell with roughened walls while simultaneously measuring the local velocity field via ultrasonic velocimetry. Results for different concentrations show that, for a specific range of shear rates just below the critical value, the observed shear band develops together with a slip layer that guarantees the sample is always sheared at the globally-imposed shear rate. Using a generalized lever rule and accounting for the different thixotropic time-scales, we can explain not only the existence of this peculiar shear-banding scenario, but also derive a logarithmic scaling law for the slip velocity that is a direct consequence of the thixotropic bulk behavior. Finally, we show that the velocity field measured at the smallest shear rates accessible can be understood in terms of non-local effects related to the finite size of the particles relative to the dimension of the shear band.