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Linear instability of planar shear banded flow
1Polymer IRC and School of Physics & Astronomy, University of Leeds, Leeds LS2 9JT, United Kingdom.
Physical Review Letters
|October 4, 2005
Summary
The nonlocal Johnson-Segalman model shows planar shear banded flow interfaces are unstable to perturbations. These instabilities grow over time, indicating a dynamic and evolving flow behavior.
Area of Science:
- Rheology and fluid dynamics
- Nonlinear continuum mechanics
Background:
- Shear banding is a common phenomenon in complex fluids, leading to the formation of distinct low- and high-strain regions.
- Understanding the stability of these bands is crucial for predicting fluid behavior under shear.
- The nonlocal Johnson-Segalman model provides a theoretical framework for studying shear banding.
Purpose of the Study:
- To investigate the linear stability of planar shear banded flow within the nonlocal Johnson-Segalman model.
- To analyze the growth of perturbations and determine the conditions for interface instability.
- To characterize the nature of the instability using unstable eigenfunctions.
Main Methods:
- Linear stability analysis of the nonlocal Johnson-Segalman model.
- Perturbation analysis with wave vectors in the plane of the banding interface.
- Numerical computation of unstable eigenfunctions.
Main Results:
- The planar shear banded flow interface is found to be linearly unstable.
- Perturbations grow over a range of wave vectors, confirming the instability.
- The study provides insights into the characteristics of the unstable eigenfunctions.
Conclusions:
- The interface in planar shear banded flow is inherently unstable under the nonlocal Johnson-Segalman model.
- The findings suggest that shear banding structures are dynamic and can evolve over time.
- Further investigation into model H stability provides context for phase-separated domains in shear flow.