Abstract
We present the results of an experimental investigation into the stability of steep interfacial waves in two immiscible liquid layers subject to horizontal oscillations. Two-dimensional waves, which arise beyond a critical forcing speed V c (product of forcing frequency and amplitude), can in turn lose stability to oscillatory transverse amplitude modulations with a near sub-harmonic response at a critical value of the forcing speed, V cs > V c. We characterize the resulting transverse waves and study the effect of viscosity on the onset of this secondary instability. Our experiments show that V cs increases with the ratio of the viscosities of the two liquids, N ≥ 1, which is in contrast to the decreasing trend of V c. The thresholds converge with decreasing N but appear to remain distinct even as N → 1. However, our results suggest a change of behavior for N ≤ 39, which also coincides with the first observations of interface breakup. © 2012 American Institute of Physics.
Original language | English |
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Article number | 044104 |
Journal | Physics of Fluids |
Volume | 24 |
Issue number | 4 |
DOIs | |
Publication status | Published - 2 Apr 2012 |