Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/79413
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dc.contributorDepartment of Mechanical Engineeringen_US
dc.creatorLuo, Xen_US
dc.creatorZhang, Fen_US
dc.creatorDing, Jen_US
dc.creatorSi, Ten_US
dc.creatorYang, Jen_US
dc.creatorZhai, Zen_US
dc.creatorWen, CYen_US
dc.date.accessioned2018-11-26T09:31:21Z-
dc.date.available2018-11-26T09:31:21Z-
dc.identifier.issn0022-1120en_US
dc.identifier.urihttp://hdl.handle.net/10397/79413-
dc.language.isoenen_US
dc.publisherCambridge University Pressen_US
dc.rights© Cambridge University Press 2018en_US
dc.rightsThis 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 in any medium, provided the original work is properly cited.en_US
dc.rightsThe following publication Luo, X., Zhang, F., Ding, J., Si, T., Yang, J., Zhai, Z., & Wen, C. (2018). Long-term effect of Rayleigh–Taylor stabilization on converging Richtmyer–Meshkov instability. Journal of Fluid Mechanics, 849, 231-244 is available at https://dx.doi.org/10.1017/jfm.2018.424en_US
dc.subjectcompressible flowsen_US
dc.subjectshock wavesen_US
dc.titleLong-term effect of Rayleigh-Taylor stabilization on converging Richtmyer-Meshkov instabilityen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage231en_US
dc.identifier.epage244en_US
dc.identifier.volume849en_US
dc.identifier.doi10.1017/jfm.2018.424en_US
dcterms.abstractThe Richtmyer-Meshkov instability on a three-dimensional single-mode light/heavy interface is experimentally studied in a converging shock tube. The converging shock tube has a slender test section so that the non-uniform feature of the shocked flow is amply exhibited in a long testing time. A deceleration phenomenon is evident in the unperturbed interface subjected to a converging shock. The single-mode interface presents three-dimensional characteristics because of its minimum surface feature, which leads to the stratified evolution of the shocked interface. For the symmetry interface, it is quantitatively found that the perturbation amplitude experiences a rapid growth to a maximum value after shock compression and finally drops quickly before the reshock. This quick reduction of the interface amplitude is ascribed to a significant Rayleigh-Taylor stabilization effect caused by the deceleration of the light/heavy interface. The long-term effect of the Rayleigh-Taylor stabilization even leads to a phase inversion on the interface before the reshock when the initial interface has sufficiently small perturbations. It is also found that the amplitude growth is strongly suppressed by the three-dimensional effect, which facilitates the occurrence of the phase inversion.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of fluid mechanics, 2018, v. 849, p. 231-244en_US
dcterms.isPartOfJournal of fluid mechanicsen_US
dcterms.issued2018-
dc.identifier.scopus2-s2.0-85048775855-
dc.identifier.eissn1469-7645en_US
dc.description.validate201811 bcmaen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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