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Downward flame spread over a thick PMMA slab in an opposed flow environment: experiment and modeling

dc.citation.epage707en_US
dc.citation.issue4en_US
dc.citation.spage697en_US
dc.citation.volume132en_US
dc.citation.woscount11
dc.contributor.authorWu, KKen_US
dc.contributor.authorFan, WFen_US
dc.contributor.authorChen, CHen_US
dc.contributor.authorLiou, TMen_US
dc.contributor.authorPan, IJen_US
dc.contributor.department機械工程學系zh_TW
dc.contributor.departmentDepartment of Mechanical Engineeringen_US
dc.date.accessioned2014-12-08T15:41:16Z
dc.date.available2014-12-08T15:41:16Z
dc.date.issued2003-03-01en_US
dc.description.abstractThis work investigates experimentally and theoretically the downward spread of a flame over a thick polymethylmethacrylate (PMMA) slab with an opposed flow of air. Simulation results, using an unsteady combustion model with mixed convection, indicate that the ignition delay time increases with a decreasing opposed-flow temperature or increasing velocity. The ignition delay time is nearly constant at a low opposed flow velocity, i.e., (u(&INFIN;)) over bar less than or equal to 30 cm/s. Experiments were conducted at three different opposed flow temperatures and velocities, namely, (T-i) over bar = 313, 333, and 353 K and (u(&INFIN;)) over bar= 40, 70, and 100 cm/s, respectively. Measurements included the flame-spread rate and temperature distributions, using thermocouples and laser-holographic interferometry. The qualitative trends of the flame-spread rate and thermal boundary layer thickness, as obtained experimentally and from numerical predictions, were identical. For a quantitative comparison, the predicted and experimental flame-spread rates correlated well with each other, except at the lowest velocity ((u(&INFIN;)) over bar = 40 cm/s). The discrepancies between the measured and predicted thermal boundary layer thicknesses decreased with an increasing flow velocity. The quantitative agreement with a high velocity indicates that the spread of an opposed flame is mainly controlled by the flame front, whereas the discrepancies at low flow rates demonstrate the importance of radiation, the finite length of the fuel, and also three-dimensional effects, which were not considered in the model. The temperature profiles around the flame front measured by interferometric photographs indicate a recirculation flow there, as predicted by the simulation. (C) 2003 The Combustion Institute. All rights reserved.en_US
dc.identifier.doi10.1016/S0010-2180(02)00520-5en_US
dc.identifier.issn0010-2180en_US
dc.identifier.journalCOMBUSTION AND FLAMEen_US
dc.identifier.urihttp://dx.doi.org/10.1016/S0010-2180(02)00520-5en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/28063
dc.identifier.wosnumberWOS:000182454600009
dc.language.isoen_USen_US
dc.subjectflame spreaden_US
dc.subjectopposed flow velocityen_US
dc.subjectopposed flow temperatureen_US
dc.titleDownward flame spread over a thick PMMA slab in an opposed flow environment: experiment and modelingen_US
dc.typeArticleen_US

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