Sound scattering by rough elongated elastic objects. II: Fluctuations of scattered field

dc.contributor.author Stanton, Timothy K.
dc.contributor.author Chu, Dezhang
dc.date.accessioned 2008-10-17T18:59:31Z
dc.date.available 2008-10-17T18:59:31Z
dc.date.issued 1992-09
dc.description Author Posting. © Acoustical Society of America, 1992. This article is posted here by permission of Acoustical Society of America for personal use, not for redistribution. The definitive version was published in Journal of the Acoustical Society of America 92 (1992): 1665-1678, doi:10.1121/1.403906. en
dc.description.abstract Sonar echoes from unresolved features of rough objects tend to interfere with each other. Because of these interferences, properties of the echoes, such as its envelope level, will vary from realization to realization of stochastically rough objects. In this article, the nature of the fluctuations of the backscattered echo envelope of rough solid elastic elongated objects is investigated. A general formulation is initially presented after which specific formulas are derived and numerically evaluated for straight finite-length cylinders. The study uses both the approximate modal-series- and Sommerfeld–Watson-transformation-based deformed cylinder solutions presented in the first part of this series [T. K. Stanton, J. Acoust. Soc. Am. 92, XXX (1992)]. The fluctuations of the backscattered echo envelope are related to the Rice probability density function (PDF) and shown to depend upon δ/a and [script L]/L in the Rayleigh scattering region (ka≪1) and kδ and [script L]/L in the geometric region (ka≫1), where δ is the rms roughness, a is the radius of the cylinder, [script L] is the correlation length of the roughness, L is the length of the cylinder, and k is the acoustic wave number in the surrounding fluid. There are similarities shown between these fluctuations in the geometric region and those from rough planar interfaces. In addition, analytical expressions and numerical examples show that the fluctuation or ``incoherent'' component of the scattered field is random only in amplitude—its phase approaches a constant value, in phase with the mean scattered field, which needed to be taken into account in the formulation. Finally, applications of the theory developed in this article to backscatter data involving live marine shrimp-like organisms are discussed. en
dc.description.sponsorship This work was supported by the U.S. Office of Naval Research Grant Nos. N00014-89-J-1729 and N00014-90-J-1804. en
dc.format.mimetype application/pdf
dc.identifier.citation Journal of the Acoustical Society of America 92 (1992): 1665-1678 en
dc.identifier.doi 10.1121/1.403906
dc.identifier.uri https://hdl.handle.net/1912/2509
dc.language.iso en_US en
dc.publisher Acoustical Society of America en
dc.relation.uri https://doi.org/10.1121/1.403906
dc.subject Sound waves en
dc.subject Backscattering en
dc.subject Fluctuations en
dc.subject Roughness en
dc.subject Cylinders en
dc.subject Interference en
dc.subject Underwater en
dc.subject Shrimp en
dc.title Sound scattering by rough elongated elastic objects. II: Fluctuations of scattered field en
dc.type Article en
dspace.entity.type Publication
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relation.isAuthorOfPublication ac9e37cc-67f7-4182-a7dd-200de5a38fb7
relation.isAuthorOfPublication.latestForDiscovery 9b4f4f6d-0551-4b7a-a128-7976b273a179
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