A three-dimensional model for acoustic scattering from rough ocean bathymetry
β Scribed by R.N. Baer; D.H. Berman; J.S. Perkins; E.B. Wright
- Publisher
- Elsevier Science
- Year
- 1985
- Tongue
- English
- Weight
- 569 KB
- Volume
- 11
- Category
- Article
- ISSN
- 0898-1221
No coin nor oath required. For personal study only.
β¦ Synopsis
Scattering of acoustic waves by rough bathymetry is an important factor influencing the performance of array systems. This paper discusses a computer model that calculates the directional distribution of bottom-scattered energy received at an array. The model simultaneously includes the effect of bathymetric scattering and refraction caused by a varying sound-speed structure in the water column. The numerical techniques used include the split-step solution to the parabolic equation approximation to the Helmholtz equation away from the boundary. propagation of the coherence function near the boundary. and a modified Kirchhoff formulation to incorporate scattering. An exponential substitution approximation. which can reduce the computation time of the scattering component by two orders of magnitude wtth little loss in accuracy, is described.
π SIMILAR VOLUMES
## Abstract Variational formulations for direct timeβharmonic scattering problems in a threeβdimensional waveguide are formulated and analyzed. We prove that the operators defined by the corresponding forms satisfy a GΓ₯rding inequality in adequately chosen spaces of test and trial functions and dep
We present a finite element model for acoustic scattering from an elastic object situated near (or intersecting) the surface separating two fluid domains, each of semi-infinite extent. The fluid domains are truncated using a perfectly matched layer (PML) formulated as an intrinsic part of the mathem
## Abstract In this article, an efficient hybrid MMβPO method combining UV technique is applied to calculate the EM scattering from a 2D PEC target above a PEC rough surface. Considering the target as the MM region and the rough surface as the PO region, the current on the rough surface is obtained