Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/106548
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dc.contributorDepartment of Mechanical Engineering-
dc.creatorYuan, Yen_US
dc.creatorZhang, Ten_US
dc.creatorYao, Wen_US
dc.creatorFan, Xen_US
dc.creatorZhang, Pen_US
dc.date.accessioned2024-05-09T00:54:11Z-
dc.date.available2024-05-09T00:54:11Z-
dc.identifier.issn1540-7489en_US
dc.identifier.urihttp://hdl.handle.net/10397/106548-
dc.language.isoenen_US
dc.publisherElsevier Inc.en_US
dc.rights©2016 The Combustion Institute. Published by Elsevier Inc. All rights reserved.en_US
dc.rights©2016 . This manuscript version is made available under the CC-BY-NC-ND 4.0 license https://creativecommons.org/licenses/by-nc-nd/4.0/en_US
dc.rightsThe following publication Yuan, Y., Zhang, T., Yao, W., Fan, X., & Zhang, P. (2017). Characterization of flame stabilization modes in an ethylene-fueled supersonic combustor using time-resolved CH∗ chemiluminescence. Proceedings of the Combustion Institute, 36(2), 2919-2925 is available at https://doi.org/10.1016/j.proci.2016.07.040.en_US
dc.subjectCH∗ chemiluminesenceen_US
dc.subjectFlame stabilizationen_US
dc.subjectGloabal equivalence ratioen_US
dc.subjectStagtnation temperatureen_US
dc.subjectSupersonic combustionen_US
dc.titleCharacterization of flame stabilization modes in an ethylene-fueled supersonic combustor using time-resolved CH* chemiluminescenceen_US
dc.typeConference Paperen_US
dc.identifier.spage2919en_US
dc.identifier.epage2925en_US
dc.identifier.volume36en_US
dc.identifier.issue2en_US
dc.identifier.doi10.1016/j.proci.2016.07.040en_US
dcterms.abstractFlame stabilization in a Ma = 2.5 direct-connect supersonic combustor was experimentally characterized with a fixed stagnation pressure of 1.0 MPa and wide ranges of stagnation temperature (T0) from 1200 K to 1800 K and global equivalence ratio (Φ) of ethylene/air from 0.1 to 0.8. Four typical flame stabilization modes were identified by using the time resolved CH* chemiluminescence and presented as a regime nomogram in the T0–Φ parameter space. As increasing T0, the range of Φ for the flame stabilization modes is widened and that for the oscillation mode is therefore narrowed. The widely used quasi-1D analysis, with the experimentally determined wall static pressure distribution as input parameters, suggests that the combustor operates in a scramjet mode when the flame is stabilized in the cavity shear layer and in a ramjet mode when the flame is in the jet-wake. The flame oscillation mode, observed only for a narrow range of Φ, was found to correlate with the combustor transition between the scramjet and ramjet modes.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationProceedings of the Combustion Institute, 2017, v. 36, no. 2, p. 2919-2925en_US
dcterms.isPartOfProceedings of the Combustion Instituteen_US
dcterms.issued2017-
dc.identifier.scopus2-s2.0-84978829783-
dc.identifier.eissn1873-2704en_US
dc.description.validate202405 bcch-
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumberME-0866-
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextNational Nature Science Foundation of China; The Hong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS6660846-
dc.description.oaCategoryGreen (AAM)en_US
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