Abstract

We study the fingering instability of the interface between two miscible fluids, a colloidal suspension and its own solvent. The temporal evolution of the interface in a Hele-Shaw cell is found to be governed by the competition between the non-linear viscosity of the suspension and an off-equilibrium, effective surface tension ΓeΓ_e. By studying suspensions in a wide range of volume fractions, ΦCΦ_\mathrm{C}, we show that Γe∼ΦC2Γ_e \sim Φ_\mathrm{C}^2, in agreement with Korteweg's theory for miscible fluids. The surface tension exhibits an anomalous increase with particle size, which we account for using entropy arguments.

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