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Transmission and reflection of internal solitary waves incident upon a triangular barrier

Published online by Cambridge University Press:  23 June 2015

B. R. Sutherland*
Affiliation:
Department of Physics, University of Alberta, Edmonton, T6G 2E1, Canada Department of Earth and Atmospheric Sciences, University of Alberta, Edmonton, T6G 2E6, Canada
S. Keating
Affiliation:
Department of Physics, University of Alberta, Edmonton, T6G 2E1, Canada
I. Shrivastava
Affiliation:
Department of Civil Engineering, IIT Bombay, Mumbai 400 076, India Department of Civil and Environmental Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139-4307, USA
*
Email address for correspondence: bruce.sutherland@ualberta.ca

Abstract

We report upon laboratory experiments and numerical simulations examining the evolution of an interfacial internal solitary wave incident upon a triangular ridge whose peak lies below the interface. If the ridge is moderately large, the wave is observed to shoal and break similar to solitary waves shoaling upon a constant slope, but interfacial waves are also observed to transmit over and reflect from the ridge. In laboratory experiments, by measuring the interface displacement as it evolves in time, we measure the relative transmission and reflection of available potential energy after the incident wave has interacted with the ridge. The numerical simulations of laboratory- and ocean-scale waves measure both the available potential and kinetic energy to determine the partition of incident energy into that which is transmitted and reflected. From shallow-water theory, we define a critical amplitude, $A_{c}$, above which interfacial waves are unstable. The transmission is found to decrease from one to zero as the ratio of the incident wave amplitude to $A_{c}$ increases from less than to greater than one. Empirical fits are made to analytic curves through measurements of the transmission and reflection coefficients.

Type
Papers
Copyright
© 2015 Cambridge University Press 

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Sutherland et al. supplementary movie

Movie corresponding to experiment shown in Figure 3a

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Sutherland et al. supplementary movie

Movie corresponding to experiment shown in Figure 3a

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Sutherland et al. supplementary movie

Movie corresponding to experiment shown in Figure 3b

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Sutherland et al. supplementary movie

Movie corresponding to experiment shown in Figure 3b

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Movie corresponding to simulation shown in figure 7

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Sutherland et al. supplementary movie

Movie corresponding to simulation shown in figure 7

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Movie corresponding to simulation shown in figure 10

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Sutherland et al. supplementary movie

Movie corresponding to simulation shown in figure 10

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