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Updated: Jun 8, 2026

Studying Large Amplitude Oscillatory Shear Response of Soft Materials
Published on: April 25, 2019
Transient shear banding in a simple yield stress fluid
Thibaut Divoux1, David Tamarii, Catherine Barentin
1Université de Lyon, Laboratoire de Physique, Ecole Normale Supérieure de Lyon, CNRS UMR 5672, 46 Allée d'Italie, 69364 Lyon cedex 07, France.
Simple yield stress fluids show temporary shear banding before stabilizing. This transient behavior follows a power law with shear rate and can persist for extended periods at low rates, explaining slow stress relaxation.
Area of Science:
- Rheology
- Soft Matter Physics
Background:
- Yield stress fluids are crucial in many industrial applications.
- Understanding their flow behavior, especially transient dynamics, is essential for process optimization.
- Simple yield stress fluids lacking aging or thixotropy provide a fundamental model system.
Purpose of the Study:
- To investigate the transient shear banding in simple yield stress fluids.
- To characterize the relationship between shear rate and the duration of the transient regime.
- To explore the influence of experimental parameters like gap width and boundary conditions.
Main Methods:
- Experimental rheometry on carbopol dispersions.
- Application of controlled shear rates.
- Observation and measurement of velocity profiles over time.
Main Results:
- Simple yield stress fluids exhibit transient shear banding before achieving a steady state with a homogeneous velocity profile.
- The duration of this transient regime follows a power-law decay with increasing shear rate.
- This power-law behavior is independent of gap width and boundary conditions for a given sample preparation.
- Heterogeneous flows were observed for up to 10^5 seconds at shear rates below 0.1 s^-1.
Conclusions:
- Transient shear banding is a fundamental characteristic of simple yield stress fluids.
- The observed power-law scaling provides a quantitative description of the transient regime duration.
- The long-lived heterogeneous flows at low shear rates are responsible for ultraslow stress relaxation phenomena.
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