Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/107791
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dc.contributorDepartment of Mechanical Engineeringen_US
dc.creatorZeng, Len_US
dc.creatorZhao, Fen_US
dc.creatorWang, Hen_US
dc.creatorLiu, Yen_US
dc.creatorTang, Hen_US
dc.date.accessioned2024-07-12T01:21:32Z-
dc.date.available2024-07-12T01:21:32Z-
dc.identifier.issn1070-6631en_US
dc.identifier.urihttp://hdl.handle.net/10397/107791-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2023 Author(s). Published under an exclusive license by AIP Publishing.en_US
dc.rightsThis article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. This article appeared in Lingwei Zeng, Fuwang Zhao, Hanfeng Wang, Yang Liu, Hui Tang; Control of flow-induced vibration of a circular cylinder using a splitter plate. Physics of Fluids 1 August 2023; 35 (8): 087104 and may be found at https://doi.org/10.1063/5.0160114.en_US
dc.titleControl of flow-induced vibration of a circular cylinder using a splitter plateen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume35en_US
dc.identifier.issue8en_US
dc.identifier.doi10.1063/5.0160114en_US
dcterms.abstractA circular cylinder attached by a rigid splitter plate of different lengths was tested to examine its effects on the control of flow-induced vibration. Tests were carried out in a closed-loop water channel. A cylinder of diameter D = 20 mm and a mass ratio m* ≈ 50 was installed to oscillate in the transverse direction. A wide range of splitter length was considered, i.e., L/D = 0-3.5, at a range of reduced velocity Ur = 1-25 and the Reynolds number Re = 800-11 000. Numerical simulations were also conducted to reveal the flow structures associated with the vibration modes observed in the experiment. It is found that, as L/D increases from 0 to 0.25, the peak value of cylinder oscillation amplitude increases and appears at higher reduced velocities. When the splitter length continues to rise, galloping-type oscillations occur at L/D = 0.5 and 0.75. The transition stage has been found at L/D = 1.0. Oscillation is then significantly suppressed when the splitter length is larger than L/D = 1.5.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationPhysics of fluids, Aug. 2023, v. 35, no. 8, 87104en_US
dcterms.isPartOfPhysics of fluidsen_US
dcterms.issued2023-08-
dc.identifier.scopus2-s2.0-85167345289-
dc.identifier.eissn1089-7666en_US
dc.identifier.artn87104en_US
dc.description.validate202407 bcwhen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumbera3005-
dc.identifier.SubFormID49153-
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextNatural Science Foundation of Guangdong Provinceen_US
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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