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Faraday instability of a two-layer liquid film with a free upper surface

Andrey Pototsky1 and Michael Bestehorn2

  • 1Department of Mathematics, Faculty of Science Engineering and Technology, Swinburne University of Technology, Hawthorn, Victoria 3122, Australia
  • 2Department of Statistical Physics and Nonlinear Dynamics, Brandenburg University of Technology, 03044 Cottbus-Senftenberg, Germany

Phys. Rev. Fluids 1, 023901 – Published 7 June, 2016

DOI: https://doi.org/10.1103/PhysRevFluids.1.023901

Abstract

We study the linear stability of a laterally extended flat two-layer liquid film under the influence of external vertical vibration. The first liquid layer rests on a vibrating solid plate and is overlaid by a second layer of immiscible fluid with deformable upper surface. Surface waves, excited as the result of the Faraday instability, can be characterized by a time-dependent relative amplitude of the displacements of the liquid-liquid and the liquid-gas interfaces. The in-phase displacements are associated with a zigzag (barotropic) mode and the antiphase displacement corresponds to the varicose thinning mode. We numerically determine the stability threshold in the vibrated two-layer film and compute the dispersion relation together with the decay rates of the surface waves in the absence of vibration. The in-phase and the antiphase displacements are strongly coupled in the vibrated system. The interplay between the Faraday and the Rayleigh-Taylor instabilities in the system with heavier fluid on top of a lighter fluid is analyzed.

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