Please use this identifier to cite or link to this item:
http://hdl.handle.net/10397/93028
| DC Field | Value | Language |
|---|---|---|
| dc.contributor | Department of Mechanical Engineering | en_US |
| dc.contributor | Department of Aeronautical and Aviation Engineering | en_US |
| dc.creator | Shi, L | en_US |
| dc.creator | Uy, KCK | en_US |
| dc.creator | Wen, CY | en_US |
| dc.date.accessioned | 2022-05-30T07:40:10Z | - |
| dc.date.available | 2022-05-30T07:40:10Z | - |
| dc.identifier.issn | 0022-1120 | en_US |
| dc.identifier.uri | http://hdl.handle.net/10397/93028 | - |
| dc.language.iso | en | en_US |
| dc.publisher | Cambridge University Press | en_US |
| dc.rights | This 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.rights | When 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.subject | Detonation waves | en_US |
| dc.title | The re-initiation mechanism of detonation diffraction in a weakly unstable gaseous mixture | en_US |
| dc.type | Journal/Magazine Article | en_US |
| dc.identifier.volume | 895 | en_US |
| dc.identifier.doi | 10.1017/jfm.2020.311 | en_US |
| dcterms.abstract | Numerical 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.accessRights | open access | en_US |
| dcterms.bibliographicCitation | Journal of fluid mechanics, 25 July 2020, v. 895, A24 | en_US |
| dcterms.isPartOf | Journal of fluid mechanics | en_US |
| dcterms.issued | 2020-07-25 | - |
| dc.identifier.scopus | 2-s2.0-85085190327 | - |
| dc.identifier.eissn | 1469-7645 | en_US |
| dc.identifier.artn | A24 | en_US |
| dc.description.validate | 202205 bchy | en_US |
| dc.description.oa | Accepted Manuscript | en_US |
| dc.identifier.FolderNumber | ME-0328 | - |
| dc.description.fundingSource | Others | en_US |
| dc.description.fundingText | State Key Laboratory of Explosion Science and Technology; Beijing Institute of Technology; National Natural Science Foundation of China | en_US |
| dc.description.pubStatus | Published | en_US |
| dc.identifier.OPUS | 21679362 | - |
| dc.description.oaCategory | Green (AAM) | en_US |
| Appears in Collections: | Journal/Magazine Article | |
Files in This Item:
| File | Description | Size | Format | |
|---|---|---|---|---|
| Shi_Re-Initiation_Mechanism_Detonation.pdf | Pre-Published version | 5.14 MB | Adobe PDF | View/Open |
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