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Properties of the acoustic intensity vector field in a shallow water waveguide

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dc.contributor.authorDall'Osto, David R.-
dc.contributor.authorDahl, Peter H.-
dc.contributor.authorChoi, Jee Woong-
dc.date.accessioned2021-06-23T07:53:44Z-
dc.date.available2021-06-23T07:53:44Z-
dc.date.created2021-01-21-
dc.date.issued2012-03-
dc.identifier.issn0001-4966-
dc.identifier.urihttps://scholarworks.bwise.kr/erica/handle/2021.sw.erica/33190-
dc.description.abstractAcoustic intensity is a vector quantity described by collocated measurements of acoustic pressure and particle velocity. In an ocean waveguide, the interaction among multipath arrivals of propagating wavefronts manifests unique behavior in the acoustic intensity. The instantaneous intensity, or energy flux, contains two components: a propagating and non-propagating energy flux. The instantaneous intensity is described by the time-dependent complex intensity, where the propagating and non-propagating energy fluxes are modulated by the active and reactive intensity envelopes, respectively. Properties of complex intensity are observed in data collected on a vertical line array during the transverse acoustic variability experiment (TAVEX) that took place in August of 2008, 17 km northeast of the Ieodo ocean research station in the East China Sea, 63 m depth. Parabolic equation (PE) simulations of the TAVEX waveguide supplement the experimental data set and provide a detailed analysis of the spatial structure of the complex intensity. A normalized intensity quantity, the pressure-intensity index, is used to describe features of the complex intensity which have a functional relationship between range and frequency, related to the waveguide invariant. The waveguide invariant is used to describe the spatial structure of intensity in the TAVEX waveguide using data taken at discrete ranges. (C) 2012 Acoustical Society of America. [DOI: 10.1121/1.3682063]-
dc.language영어-
dc.language.isoen-
dc.publisherAcoustical Society of America-
dc.titleProperties of the acoustic intensity vector field in a shallow water waveguide-
dc.typeArticle-
dc.contributor.affiliatedAuthorChoi, Jee Woong-
dc.identifier.doi10.1121/1.3682063-
dc.identifier.scopusid2-s2.0-84858965579-
dc.identifier.wosid000301719200032-
dc.identifier.bibliographicCitationJournal of the Acoustical Society of America, v.131, no.3, pp.2023 - 2035-
dc.relation.isPartOfJournal of the Acoustical Society of America-
dc.citation.titleJournal of the Acoustical Society of America-
dc.citation.volume131-
dc.citation.number3-
dc.citation.startPage2023-
dc.citation.endPage2035-
dc.type.rimsART-
dc.type.docTypeArticle-
dc.description.journalClass1-
dc.description.isOpenAccessN-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaAcoustics-
dc.relation.journalResearchAreaAudiology & Speech-Language Pathology-
dc.relation.journalWebOfScienceCategoryAcoustics-
dc.relation.journalWebOfScienceCategoryAudiology & Speech-Language Pathology-
dc.subject.keywordAuthoracoustic arrays-
dc.subject.keywordAuthoracoustic intensity-
dc.subject.keywordAuthoracoustic waveguides-
dc.subject.keywordAuthorparabolic equations-
dc.subject.keywordAuthorunderwater acoustic propagation-
dc.identifier.urlhttps://asa.scitation.org/doi/10.1121/1.3682063-
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