2006
DOI: 10.1121/1.2141265
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Broadband modeling of downslope propagation in a penetrable wedge

Abstract: Sound propagation in a wedge-shaped environment with a penetrable bottom is simulated with broadband adiabatic mode, coupled mode, and parabolic equation model computations. Simulated results are compared to measured data taken in a tank experiment by Tindle et al. The coupled mode formalism is shown to predict, in agreement with that experiment, that modal wave fronts in penetrable wedges are approximately circular arcs centered at the apex of the wedge for a source near the apex. It is also shown that for we… Show more

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Cited by 6 publications
(2 citation statements)
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“…makes the problem an improper Sturm-Liouville type. 26 In the limit that the false bottom approaches infinity this solution is equivalent to either the Pekeris cut approach or the EJP cut approach. For either choice, there are trapped modes plus a contour integral deformed to lie along the respective branch line that must be evaluated.…”
Section: Introductionmentioning
confidence: 98%
“…makes the problem an improper Sturm-Liouville type. 26 In the limit that the false bottom approaches infinity this solution is equivalent to either the Pekeris cut approach or the EJP cut approach. For either choice, there are trapped modes plus a contour integral deformed to lie along the respective branch line that must be evaluated.…”
Section: Introductionmentioning
confidence: 98%
“…Previously, the two-way integral equation coupled-mode (IECM) approach has proved successful, when an adiabatic approach is not applicable, in producing benchmark solutions of the total pressure field as a function of range in the forward direction for large scale, i.e., smooth, range-dependent boundaries that result in forward-and back-scattering from mode coupling. [3][4][5][6] The goal of this paper is to establish a benchmark solution that is, in principle, an exact numerical solution for the reverberation time series for an environment with a range-dependent fine-scale rough bottom boundary that induces mode coupling and generates a scattered field. The solution includes scattering effects to all orders, i.e., sums the infinite series of forward and backward contributions at each range point and maintains energy conservation.…”
Section: Introductionmentioning
confidence: 99%