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dc.contributor.authorLi, Zhong
dc.contributor.authorAbrahamsen-Prsic, Mia
dc.contributor.authorOng, Muk Chen
dc.contributor.authorKhoo, Boo Cheong
dc.date.accessioned2019-01-08T10:31:21Z
dc.date.available2019-01-08T10:31:21Z
dc.date.created2018-07-04T13:45:54Z
dc.date.issued2018
dc.identifier.citationJournal of Fluids and Structures. 2018, 76 251-271.nb_NO
dc.identifier.issn0889-9746
dc.identifier.urihttp://hdl.handle.net/11250/2579630
dc.description.abstractLarge Eddy Simulations (LES) with Smagorinsky subgrid scale model have been performed for the flow past two circular cylinders in tandem placed in the vicinity of a horizontal plane wall at very small gap ratios, namely G/D = 0.1, 0.3 and 0.5, in three-dimension (3D). The ratio of cylinder center-to-center distance to cylinder diameter, or the pitch ratio, L/D, considered in the simulations is L/D = 2 and 5. This work serves as an extension of Abrahamsen Prsic et al. (2015) [1]. In essence, six sets of simulations have been performed in the subcritical Reynolds number regime at Re = 1.31 × 104 . Our major findings can be summarized as follows. (1) At both pitch ratios, the wall proximity has a decreasing effect on the mean drag coefficient of the upstream cylinder. At L/D = 2, the mean drag coefficient of the downstream cylinder is negative since it is located within the drag inversion separation distance. (2) At L/D = 2, a squarish cavity-like flow exists between the cylinders and the flow circulates within the cavity. A long lee-wake recirculation zone is found behind the downstream cylinder at G/D = 0.1. However, a much smaller lee-wake recirculation zone is noticed at L/D = 5 with G/D = 0.1. (3) At L/D = 2, the reattachment is biased to the bottom shear layer due to the deflection from the plane wall, which leads to the formation of the slanted squarish cavity-like flow. At both pitch ratios, as G/D becomes smaller, stronger vortices are found between the two cylinders. Vortices of less intensity are observed in the near wake of the downstream cylinder due to the vortex shedding suppression of the neighbouring wall.nb_NO
dc.language.isoengnb_NO
dc.publisherElseviernb_NO
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/deed.no*
dc.titleLarge Eddy Simulations of flow around two circular cylinders in tandem in the vicinity of a plane wall at small gap ratiosnb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionacceptedVersionnb_NO
dc.source.pagenumber251-271nb_NO
dc.source.volume76nb_NO
dc.source.journalJournal of Fluids and Structuresnb_NO
dc.identifier.doi10.1016/j.jfluidstructs.2017.10.006
dc.identifier.cristin1595657
dc.description.localcode© 2017. This is the authors’ accepted and refereed manuscript to the article. Locked until 2.11.2019 due to copyright restrictions. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/nb_NO
cristin.unitcode194,64,20,0
cristin.unitnameInstitutt for marin teknikk
cristin.ispublishedtrue
cristin.fulltextpostprint
cristin.qualitycode1


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Attribution-NonCommercial-NoDerivatives 4.0 Internasjonal
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