Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/111535
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dc.contributorDepartment of Mechanical Engineering-
dc.creatorHuang, L-
dc.date.accessioned2025-03-03T06:01:43Z-
dc.date.available2025-03-03T06:01:43Z-
dc.identifier.issn0001-4966-
dc.identifier.urihttp://hdl.handle.net/10397/111535-
dc.language.isoenen_US
dc.publisherAIP Publishing LLCen_US
dc.rights© 2006 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 Lixi Huang; Broadband sound reflection by plates covering side-branch cavities in a duct. J. Acoust. Soc. Am. 1 May 2006; 119 (5): 2628–2638 and may be found at https://doi.org/10.1121/1.2186431.en_US
dc.titleBroadband sound reflection by plates covering side-branch cavities in a ducten_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage2628-
dc.identifier.epage2638-
dc.identifier.volume119-
dc.identifier.issue5-
dc.identifier.doi10.1121/1.2186431-
dcterms.abstractWhen a segment of a rigid duct is replaced by a plate backed by a hard-walled cavity, grazing incident sound waves induce plate bending, hence sound reflection. The mechanism is similar to the drumlike silencer with tensioned membranes [L. Huang, J. Acoust. Soc. Am. 112, 2014–2025 (2002)]. However, the logarithmic bandwidth over which the reflection occurs is much wider than that of a drumlike silencer of the same cavity geometry, the typical difference being nearly one octave band. The difference in the silencing performance is explained in terms of the intermodal acoustic interference between the odd and even in vacuo vibration modes. For a given cavity volume, the widest stopband for noise in air is obtained by using long plates with two free lateral edges parallel with the duct axis. The optimal material should be stiff and light, and the critical parameter is found to be the ratio of the Young’s modulus over the cube of density. Typically, this ratio is 250 times higher than those of common metallic materials like aluminum alloys, but it is within the reach of existing ultralight foam materials or composite beams with a light core.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of the Acoustical Society of America, May 2006, v. 119, no. 5, p. 2628-2638-
dcterms.isPartOfJournal of the Acoustical Society of America-
dcterms.issued2006-05-
dc.identifier.scopus2-s2.0-33646464549-
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.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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