Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/89528
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dc.contributorDepartment of Building Services Engineering-
dc.creatorHuang, Xen_US
dc.creatorLink, Sen_US
dc.creatorRodriguez, Aen_US
dc.creatorThomsen, Men_US
dc.creatorOlson, Sen_US
dc.creatorFerkul, Pen_US
dc.creatorFernandez-Pello, Cen_US
dc.date.accessioned2021-04-09T08:50:24Z-
dc.date.available2021-04-09T08:50:24Z-
dc.identifier.issn1540-7489en_US
dc.identifier.urihttp://hdl.handle.net/10397/89528-
dc.language.isoenen_US
dc.publisherElsevieren_US
dc.rights© 2018 The Combustion Institute. Published by Elsevier Inc. All rights reserved.en US
dc.rights© 2018. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/.en US
dc.rightsThe following publication Huang, X., Link, S., Rodriguez, A., Thomsen, M., Olson, S., Ferkul, P., & Fernandez-Pello, C. (2019). Transition from opposed flame spread to fuel regression and blow off: Effect of flow, atmosphere, and microgravity. Proceedings of the Combustion Institute, 37(3), 4117-4126 is available at https://doi.org/10.1016/j.proci.2018.06.022.en US
dc.subjectBlue flame sheeten_US
dc.subjectBurningen_US
dc.subjectPMMA roden_US
dc.subjectReduced pressureen_US
dc.subjectRegression angleen_US
dc.titleTransition from opposed flame spread to fuel regression and blow off : effect of flow, atmosphere, and microgravityen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage4117en_US
dc.identifier.epage4126en_US
dc.identifier.volume37en_US
dc.identifier.issue3en_US
dc.identifier.doi10.1016/j.proci.2018.06.022en_US
dcterms.abstractThe spread of flames over the surface of solid combustible material in an opposed flow is different from the mass burning (or fuel regression) in a pool fire. However, the progress of a flame front over a solid fuel includes both flame spread and fuel regression, but the difference between these two processes has not been well clarified. In this work, experiments using cylindrical PMMA samples were conducted in normal gravity and in microgravity. We aim to identify the transition from opposed flame spread to fuel regression under varying conditions, including sample size, opposed flow velocity, pressure, oxygen concentration, external radiation, and gravity level. For a thick rod in normal gravity, as the opposed flow increases to 50-100 cm/s, the flame can no longer spread over the fuel surface but stay in the recirculation zone downstream of the cylinder end surface, like a pool fire flame. The flame spread first transitions to fuel regression at a critical leading-edge regression angle of α 45°, and then, flame blow-off occurs. Under large opposed flow velocity, a stable flat blue flame is formed floating above the rod end surface, because of vortex shedding. In microgravity at a low opposed flow (<10 cm/s), pure fuel regression was not observed. This work aims to clarify the differences between the flame spread and fuel regression in the progress of a flame and provide a better understanding of the blow-off phenomenon on solid fuels.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationProceedings of the Combustion Institute, 2019, v. 37, no. 3, p. 4117-4126en_US
dcterms.isPartOfProceedings of the Combustion Instituteen_US
dcterms.issued2019-
dc.identifier.scopus2-s2.0-85049186856-
dc.description.validate202104 bcvc-
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumbera0685-n03-
dc.identifier.SubFormID988-
dc.description.fundingSourceSelf-funded-
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryGreen (AAM)en_US
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