Saffman-Taylor finger width at low interfacial tension

Abstract
High-accuracy numerical results are shown which go against current conjecture that dimensionless finger width λ in the Saffman-Taylor problem is a monotonically increasing function of dimensionless surface tension τ, asymptotically approaching 1/2 as τ→0. Specifically, quasi steady-state fingers are shown for finite τ with λ significantly below 0.5. These solutions are consistent with published experimental results obtained in a Hele-Shaw cell, indicating that the Saffman-Taylor equations are sufficient to explain this phenomenon.

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