Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/104933
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dc.contributorDepartment of Aeronautical and Aviation Engineeringen_US
dc.creatorYu, Ken_US
dc.creatorHao, Jen_US
dc.creatorWen, CYen_US
dc.creatorXu, Jen_US
dc.date.accessioned2024-03-07T08:50:23Z-
dc.date.available2024-03-07T08:50:23Z-
dc.identifier.issn0022-1120en_US
dc.identifier.urihttp://hdl.handle.net/10397/104933-
dc.language.isoenen_US
dc.publisherCambridge University Pressen_US
dc.rights© The Author(s), 2024. Published by Cambridge University Press. This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (http://creativecommons.org/licenses/by/4.0), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited.en_US
dc.rightsThe following publication Yu, K., Hao, J., Wen, C. Y., & Xu, J. (2024). Bi-global stability of supersonic backward-facing step flow. Journal of Fluid Mechanics, 981, A29 is available at https://doi.org/10.1017/jfm.2024.76.en_US
dc.subjectAbsolute/convective instabilityen_US
dc.subjectSeparated flowsen_US
dc.subjectSupersonic flowen_US
dc.titleBi-global stability of supersonic backward-facing step flowen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume981en_US
dc.identifier.doi10.1017/jfm.2024.76en_US
dcterms.abstractSupersonic backward-facing step (BFS) flow is numerically studied using direct numerical simulation (DNS) and global stability analysis (GSA) with a free stream Mach number of 2.16 and a Reynolds number of 7.938 × 105 based on the flat-plate length L and free stream conditions. Two-dimensional BFS flow becomes unstable to three-dimensional perturbations as the step height h exceeds a certain value, while no two-dimensionally unstable mode is found. Global instability occurs with the fragmentation of the primary separation vortex downstream of the step. Two stationary modes and one oscillatory unstable mode are obtained at a supercritical ratio of L/h = 32.14, among which the two stationary modes originate from the coalescence of a pair of conjugate modes. The most unstable mode manifests itself as streamwise streaks in the reattached boundary layer, which is similar to that in shock-induced separated flow, although the flow separation mechanisms are different. Without introducing any external disturbances, the DNS captures the preferred perturbations and produces a growth rate in agreement with the GSA prediction in the linear growth stage. In the quasi-steady stage, the secondary separation vortex breaks up into several small bubbles, and the number of streamwise streaks is doubled. A low-frequency unsteadiness that may be associated with the oscillatory mode is also present.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of fluid mechanics, 25 Feb. 2024, v. 981, A29en_US
dcterms.isPartOfJournal of fluid mechanicsen_US
dcterms.issued2024-02-25-
dc.identifier.eissn1469-7645en_US
dc.identifier.artnA29en_US
dc.description.validate202403 bckwen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_TA-
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextNational Natural Science Foundation of China; Hong Kong Scholars Programen_US
dc.description.pubStatusPublisheden_US
dc.description.TACUP (2024)en_US
dc.description.oaCategoryTAen_US
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