Faraday resonance in a two-liquid layer system

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© 1995 The Japan Society of Fluid Mechanics and IOP Publishing Ltd
, , Citation S C Generalis and M Nagata 1995 Fluid Dyn. Res. 15 145 DOI 10.1016/0169-5983(94)00035-X

1873-7005/15/3/145

Abstract

We consider resonating wave interactions in a vertically oscillating rectangular box, which carries two liquids of different densities. The natural frequencies ω1 and ω2 of the system are assumed to satisfy the resonant condition 2ω1 = ω2 = Ω, where Ω is the frequency of the vertical vibration of the box. To study this interaction we have obtained amplitude equations which approximate the behaviour of the system in the region in parameter space where the 2ω1/Ω = 1 and ω2/Ω = 1 Mathieu instability regions cross. Our system can be transformed to that of Gu and Sethna (1987), who analysed the problem of Faraday resonance in the case of a single liquid in a rectangular container. We complement their results to quadratic order an extend them by including cubic order interactions. In particular, the results of our study show the importance of cubic order terms for second harmonic resonance, especially when dissipation is small. We choose a certain range in parameter space in order to make comparisons with previous results (Gu and Sethna 1987) and present the sequences of bifurcations and regions of chaotic behaviour for this interaction.

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10.1016/0169-5983(94)00035-X