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dc.contributorDepartment of Mechanical Engineeringen_US
dc.contributorDepartment of Aeronautical and Aviation Engineeringen_US
dc.creatorShi, Len_US
dc.creatorUy, KCKen_US
dc.creatorWen, CYen_US
dc.date.accessioned2022-05-30T07:40:10Z-
dc.date.available2022-05-30T07:40:10Z-
dc.identifier.issn0022-1120en_US
dc.identifier.urihttp://hdl.handle.net/10397/93028-
dc.language.isoenen_US
dc.publisherCambridge University Pressen_US
dc.rightsThis article has been published in a revised form in Journal of Fluid Mechanics [http://doi.org/10.1017/jfm.2020.311]. This version is free to view and download for private research and study only. Not for re-distribution or re-use. © The Author(s), 2020.en_US
dc.rightsWhen citing an Accepted Manuscript or an earlier version of an article, the Cambridge University Press requests that readers also cite the Version of Record with a DOI link. The article is subsequently published in revised form in Journal of Fluid Mechanics [http://doi.org/10.1017/jfm.2020.311].en_US
dc.subjectDetonation wavesen_US
dc.titleThe re-initiation mechanism of detonation diffraction in a weakly unstable gaseous mixtureen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume895en_US
dc.identifier.doi10.1017/jfm.2020.311en_US
dcterms.abstractNumerical simulations were performed to investigate the re-initiation mechanism of a diffracted detonation wave near the critical channel width for a weakly unstable gas. Two scenarios were examined: diffraction of a planar detonation wave and of a cellular detonation wave inside the inlet channel. The results revealed that the critical channel width predicted using a cellular detonation wave is smaller than that predicted using a planar detonation wave. The re-initiation mechanisms are described in detail by tracing massless particles along both the plane of symmetry and the re-initiation path. For planar detonation diffractions, a compression wave is formed in the far field behind the diffracted shock. Re-initiation is closely related to the amplification of this compression wave and its coalescence with the diffracted shock. Depending on the inlet channel width, the strength of the reflected rarefaction wave is responsible for weakening the strength of the compression wave and its coalescence with the diffracted shock, consequently hindering the reaction of particles behind the diffracted shock wave. In cellular cases, the continuous collisions of transverse waves, which generate local explosion sites, sustain detonation wave propagation.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of fluid mechanics, 25 July 2020, v. 895, A24en_US
dcterms.isPartOfJournal of fluid mechanicsen_US
dcterms.issued2020-07-25-
dc.identifier.scopus2-s2.0-85085190327-
dc.identifier.eissn1469-7645en_US
dc.identifier.artnA24en_US
dc.description.validate202205 bchyen_US
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumberME-0328-
dc.description.fundingSourceOthersen_US
dc.description.fundingTextState Key Laboratory of Explosion Science and Technology; Beijing Institute of Technology; National Natural Science Foundation of Chinaen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS21679362-
dc.description.oaCategoryGreen (AAM)en_US
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