Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/111494
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dc.contributorDepartment of Mechanical Engineering-
dc.creatorYang, C-
dc.creatorPan, J-
dc.creatorCheng, L-
dc.date.accessioned2025-03-03T06:01:24Z-
dc.date.available2025-03-03T06:01:24Z-
dc.identifier.issn0001-4966-
dc.identifier.urihttp://hdl.handle.net/10397/111494-
dc.language.isoenen_US
dc.publisherAIP Publishing LLCen_US
dc.rights© 2013 Acoustical Society of America. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the Acoustical Society of America.en_US
dc.rightsThe following article appeared in Cheng Yang, Jie Pan, Li Cheng; A mechanism study of sound wave-trapping barriers. J. Acoust. Soc. Am. 1 September 2013; 134 (3): 1960–1969 and may be found at https://doi.org/10.1121/1.4816542.en_US
dc.titleA mechanism study of sound wave-trapping barriersen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1960-
dc.identifier.epage1969-
dc.identifier.volume134-
dc.identifier.issue3-
dc.identifier.doi10.1121/1.4816542-
dcterms.abstractThe performance of a sound barrier is usually degraded if a large reflecting surface is placed on the source side. A wave-trapping barrier (WTB), with its inner surface covered by wedge-shaped structures, has been proposed to confine waves within the area between the barrier and the reflecting surface, and thus improve the performance. In this paper, the deterioration in performance of a conventional sound barrier due to the reflecting surface is first explained in terms of the resonance effect of the trapped modes. At each resonance frequency, a strong and mode-controlled sound field is generated by the noise source both within and in the vicinity outside the region bounded by the sound barrier and the reflecting surface. It is found that the peak sound pressures in the barrier's shadow zone, which correspond to the minimum values in the barrier's insertion loss, are largely determined by the resonance frequencies and by the shapes and losses of the trapped modes. These peak pressures usually result in high sound intensity component impinging normal to the barrier surface near the top. The WTB can alter the sound wave diffraction at the top of the barrier if the wavelengths of the sound wave are comparable or smaller than the dimensions of the wedge. In this case, the modified barrier profile is capable of re-organizing the pressure distribution within the bounded domain and altering the acoustic properties near the top of the sound barrier.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of the Acoustical Society of America, Sept 2013, v. 134, no. 3, p. 1960-1969-
dcterms.isPartOfJournal of the Acoustical Society of America-
dcterms.issued2013-09-
dc.identifier.scopus2-s2.0-84883360988-
dc.identifier.pmid23967929-
dc.identifier.eissn1520-8524-
dc.description.validate202503 bcch-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_Othersen_US
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextHong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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