Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/6626
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dc.contributorDepartment of Mechanical Engineering-
dc.creatorLam, GCY-
dc.creatorLeung, RCK-
dc.creatorTang, SK-
dc.date.accessioned2014-12-11T08:25:24Z-
dc.date.available2014-12-11T08:25:24Z-
dc.identifier.issn0001-4966-
dc.identifier.urihttp://hdl.handle.net/10397/6626-
dc.language.isoenen_US
dc.publisherAcoustical Society of Americaen_US
dc.rightsCopyright 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 Lam, G. C. Y., Leung, R. C. K., & Tang, S. K. (2013). Aeroacoustics of T-junction merging flow. Journal of the Acoustical Society of America, 133(2), 697-708 and may be found at http://scitation.aip.org/content/asa/journal/jasa/133/2/10.1121/1.4773351.en_US
dc.subjectAeroacousticsen_US
dc.subjectNavier Stokes equationsen_US
dc.subjectReynolds numberen_US
dc.titleAeroacoustics of T-junction merging flowen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: S. K. Tangen_US
dc.identifier.spage697-
dc.identifier.epage708-
dc.identifier.volume133-
dc.identifier.issue2-
dc.identifier.doi10.1121/1.4773351-
dcterms.abstractThis paper reports a numerical study of the aeroacoustics of merging flow at T-junction. The primary focus is to elucidate the acoustic generation by the flow unsteadiness. The study is conducted by performing direct aeroacoustic simulation approach, which solves the unsteady compressible Navier-Stokes equations and the perfect gas equation of state simultaneously using the conservation element and solution element method. For practical flows, the Reynolds number based on duct width is usually quite high (>10⁵). In order to properly account for the effects of flow turbulence, a large eddy simulation methodology together with a wall modeling derived from the classical logarithm wall law is adopted. The numerical simulations are performed in two dimensions and the acoustic generation physics at different ratios of side-branch to main duct flow velocities VR (=0.5,0.67,1.0,2.0) are studied. Both the levels of unsteady interactions of merging flow structures and the efficiency of acoustic generation are observed to increase with VR. Based on Curle's analogy, the major acoustic source is found to be the fluctuating wall pressure induced by the flow unsteadiness occurred in the downstream branch. A scaling between the wall fluctuating force and the efficiency of the acoustic generation is also derived.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of the Acoustical Society of America, Feb. 2013, v. 133, no. 2, p. 697-708-
dcterms.isPartOfJournal of the Acoustical Society of America-
dcterms.issued2013-02-
dc.identifier.isiWOS:000314267200019-
dc.identifier.scopus2-s2.0-84873355223-
dc.identifier.eissn1520-8524-
dc.identifier.rosgroupidr64533-
dc.description.ros2012-2013 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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