Journal of Fluid Mechanics· 2026Q1
Revisiting creeping viscoelastic cross-slot flow: global linear stability and structural sensitivity analyses
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- Q1SCImago
- 2026year
Short summary
Creeping viscoelastic cross-slot flow instability originates from elastic energy release in narrow high-extension-rate ridges, not sharp corners or a central stagnation point.
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Key points
- Viscoelastic instability in 2D creeping cross-slot flow is reproduced via direct numerical simulations and global stability analysis.
- The leading eigenmode involves a chiral velocity-stress perturbation that tilts and rotates the birefringent strand.
- Structural sensitivity and energy-budget analyses pinpoint narrow high-extension-rate ridges as the instability's core and energy source.
- Instability originates from elastic energy release in extension-dominated regions, independent of sharp corners or a free central stagnation point.
AI-generated from the title and abstract; the full text is not read.
Abstract
The viscoelastic instability of cross-slot flow was first observed experimentally almost half a century ago and reproduced numerically two decades ago, yet its physical origin remains unresolved. We revisit this problem for two-dimensional creeping flow of Oldroyd-B fluid by combining direct numerical simulations, global stability analysis, structural sensitivity analysis and energy-budget analysis. Our simulations reproduce the canonical pitchfork bifurcation, and the stability analysis consistently predicts the threshold and perturbation growth rates. The leading eigenmode consists of a chiral velocity–stress perturbation that tilts and rotates the birefringent strand generated by the extensional flow. Structural sensitivity and energy-budget analyses identify narrow high-extension-rate ridges within the extensional flow as both the spatial core and energetic source of the instability. In these ridges, the stress-based wavemaker colocalizes with large positive disturbance polymeric stress power density, indicating localized transfer of stored elastic energy to the disturbance flow. Analyses of cross-slot variants with rounded corners and with a centred cylinder further reveal that neither sharp corners nor a free central stagnation point is the essential destabilizing ingredient; rather, the instability originates from elastic-energy release in extension-dominated regions characteristic of cross-slot flow.
The authors' abstract, as published at the source. Journal of Fluid Mechanics, 2026 · DOI ↗
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Fluid Flow and Transfer ProcessesChemical Engineering