Linear instability of planar shear banded flow of both diffusive and non-diffusive Johnson-Segalman fluids
H. J. Wilson, S. M. Fielding

TL;DR
This paper analytically investigates the linear stability of shear banded planar Couette flow in Johnson-Segalman fluids, revealing long-wave instabilities in both diffusive and non-diffusive cases, with weak diffusion slightly stabilizing the flow.
Contribution
It provides the first full analytical study of shear banding flow instability, connecting long-wave instability mechanisms to experimental observations.
Findings
Flow is unstable to long waves in non-diffusive Johnson-Segalman fluids.
Weak diffusion slightly stabilizes long-wave instabilities.
Long-wave instability persists even with diffusion, relevant to experimental complex dynamics.
Abstract
We consider the linear stability of shear banded planar Couette flow of the Johnson-Segalman fluid, with and without the addition of stress diffusion to regularise the equations. In particular, we investigate the effect of two-dimensional perturbations representing undulations along the interface between shear bands. We demonstrate analytically that, for the linear stability problem, the limit in which diffusion tends to zero is mathematically equivalent to a pure (non-diffusive) Johnson-Segalman model with a material interface between the shear bands, provided the wavelength of perturbations being considered is long relative to the (short) diffusion lengthscale. For no diffusion, we find that the flow is unstable to long waves for almost all arrangements of the two shear bands. Weak diffusion provides a small stabilising effect, rendering extremely long waves marginally stable.…
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