Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/94259
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dc.contributorDepartment of Mechanical Engineeringen_US
dc.creatorWang, Cen_US
dc.creatorTang, Hen_US
dc.date.accessioned2022-08-11T01:09:44Z-
dc.date.available2022-08-11T01:09:44Z-
dc.identifier.issn0889-9746en_US
dc.identifier.urihttp://hdl.handle.net/10397/94259-
dc.language.isoenen_US
dc.publisherAcademic Pressen_US
dc.rights© 2019 Elsevier Ltd. All rights reserved.en_US
dc.rights© 2019. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/.en_US
dc.rightsThe following publication Wang, C., & Tang, H. (2019). On the aeroelastic energy transfer from a Lamb dipole to a flexible cantilever. Journal of Fluids and Structures, 86, 170-184 is available at https://doi.org/10.1016/j.jfluidstructs.2019.02.006.en_US
dc.subjectEnergy transferen_US
dc.subjectFluid–structure interactionen_US
dc.subjectLamb dipoleen_US
dc.subjectVortex dynamicsen_US
dc.titleOn the aeroelastic energy transfer from a Lamb dipole to a flexible cantileveren_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage170en_US
dc.identifier.epage184en_US
dc.identifier.volume86en_US
dc.identifier.doi10.1016/j.jfluidstructs.2019.02.006en_US
dcterms.abstractThis paper studies the aeroelastic energy transfer from an advecting Lamb dipole to a flexible cantilever. The cantilever is initially placed either along or against the dipole's advection direction with various lateral distances. As the dipole moves towards the cantilever, they interact and exchange the energy. Such a fluid–structure interaction problem is numerically solved at a low Reynolds number of 200 using a lattice Boltzmann method based numerical framework. The simulation results confirm that, when the lateral distance is around the dipole radius, placing the cantilever against the dipole's advection direction is more favorable for energy transfer. Under this setting, the cantilever generally experiences two notable increases in its mechanical energy. The first one is caused by the direct impact associated with the dipole's approach, whereas the second one occurs when the dipole just passes by and exerts suction on the cantilever's free end. Each increase leads to a peak, and the second peak is much larger representing the maximum transferred energy. It is further found that when the lateral distance is about a half of the dipole radius, the cantilever's length is about one dipole radius, and its bending stiffness is moderate, the aeroelastic efficiency can be as high as 10.6%.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of fluids and structures, Apr. 2019, v. 86, p. 170-184en_US
dcterms.isPartOfJournal of fluids and structuresen_US
dcterms.issued2019-04-
dc.identifier.scopus2-s2.0-85062067126-
dc.identifier.eissn1095-8622en_US
dc.description.validate202208 bchyen_US
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumberME-0482-
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextThe Hong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS20524792-
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