Inertial enhancement of the polymer diffusive instability

Beneitez et al. (Phys. Rev. Fluids, 8, L101901, 2023) have recently discovered a new linear "polymer diffusive instability" (PDI) in inertialess rectilinear viscoelastic shear flow using the FENE-P model when polymer stress diffusion is present. Here, we examine the impact of inertia on th...

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Bibliographic Details
Published in:arXiv.org 2024-02
Main Authors: Couchman, Miles M P, Beneitez, Miguel, Page, Jacob, Kerswell, Rich R
Format: Article
Language:English
Subjects:
Algorithms
Constitutive models
Constitutive relationships
Flow stability
Fluid flow
Inertia
Mathematical models
Parameters
Polymers
Reynolds number
Shear flow
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Summary:Beneitez et al. (Phys. Rev. Fluids, 8, L101901, 2023) have recently discovered a new linear "polymer diffusive instability" (PDI) in inertialess rectilinear viscoelastic shear flow using the FENE-P model when polymer stress diffusion is present. Here, we examine the impact of inertia on the PDI for both plane Couette (PCF) and plane Poiseuille (PPF) flows under varying Weissenberg number \(W\), polymer stress diffusivity \(\varepsilon\), solvent-to-total viscosity ratio \(\beta\), and Reynolds number \(Re\), considering the FENE-P and simpler Oldroyd-B constitutive relations. Both the prevalence of the instability in parameter space and the associated growth rates are found to significantly increase with \(Re\). For instance, as \(Re\) increases with \(\beta\) fixed, the instability emerges at progressively lower values of \(W\) and \(\varepsilon\) than in the inertialess limit, and the associated growth rates increase linearly with \(Re\) when all other parameters are fixed. For finite \(Re\), it is also demonstrated that the Schmidt number \(Sc=1/(\varepsilon Re)\) collapses curves of neutral stability obtained across various \(Re\) and \(\varepsilon\). The observed strengthening of PDI with inertia and the fact that stress diffusion is always present in time-stepping algorithms, either implicitly as part of the scheme or explicitly as a stabiliser, implies that the instability is likely operative in computational work using the popular Oldroyd-B and FENE-P constitutive models. The fundamental question now is whether PDI is physical and observable in experiments, or is instead an artifact of the constitutive models that must be suppressed.
ISSN:2331-8422
DOI:10.48550/arxiv.2308.14879