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Interactions of large amplitude solitary waves in viscous fluid conduits
Published online by Cambridge University Press: 11 June 2014
Abstract
The free interface separating an exterior, viscous fluid from an intrusive conduit of buoyant, less viscous fluid is known to support strongly nonlinear solitary waves due to a balance between viscosity-induced dispersion and buoyancy-induced nonlinearity. The overtaking, pairwise interaction of weakly nonlinear solitary waves has been classified theoretically for the Korteweg–de Vries equation and experimentally in the context of shallow water waves, but a theoretical and experimental classification of strongly nonlinear solitary wave interactions is lacking. The interactions of large amplitude solitary waves in viscous fluid conduits, a model physical system for the study of one-dimensional, truly dissipationless, dispersive nonlinear waves, are classified. Using a combined numerical and experimental approach, three classes of nonlinear interaction behaviour are identified: purely bimodal, purely unimodal, and a mixed type. The magnitude of the dispersive radiation due to solitary wave interactions is quantified numerically and observed to be beyond the sensitivity of our experiments, suggesting that conduit solitary waves behave as ‘physical solitons’. Experimental data are shown to be in excellent agreement with numerical simulations of the reduced model. Experimental movies are available with the online version of the paper.
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- © 2014 Cambridge University Press
References
Lowman et al. supplementary movie
Bimodal interaction, zoomed in and rescaled. Corresponds to the bimodal interaction in Fig. 4.
Lowman et al. supplementary movie
Bimodal interaction, zoomed in and unscaled. Corresponds to the bimodal interaction in Fig. 4.
Lowman et al. supplementary movie
Intermediate interaction, zoomed in and rescaled. Corresponds to the intermediate interaction in Fig. 4.
Lowman et al. supplementary movie
Intermediate interaction, zoomed in and unscaled. Corresponds to the intermediate interaction in Fig. 4.
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