Please use this identifier to cite or link to this item: https://doi.org/10.1016/j.fuel.2019.116809
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dc.titleModelling n-heptane dilute spray flames in a model supersonic combustor fueled by hydrogen
dc.contributor.authorHuang, Zhiwei
dc.contributor.authorZhao, Majie
dc.contributor.authorZhang, Huangwei
dc.date.accessioned2020-08-19T03:55:29Z
dc.date.available2020-08-19T03:55:29Z
dc.date.issued2020-03-15
dc.identifier.citationHuang, Zhiwei, Zhao, Majie, Zhang, Huangwei (2020-03-15). Modelling n-heptane dilute spray flames in a model supersonic combustor fueled by hydrogen. FUEL 264. ScholarBank@NUS Repository. https://doi.org/10.1016/j.fuel.2019.116809
dc.identifier.issn00162361
dc.identifier.issn18737153
dc.identifier.urihttps://scholarbank.nus.edu.sg/handle/10635/173122
dc.description.abstract© 2019 Elsevier Ltd Combustion characteristics of n-heptane dilute sprays in a model supersonic combustor fueled by hydrogen are numerically investigated. The two-phase compressible reactive flows are solved by a Eulerian-Lagrangian framework. Supersonic air enters the combustor at Mach 2.0, whereas hydrogen is injected sonically at the strut base. Monodispersed liquid n-heptane droplets are carried by hydrogen jet at different Spray Equivalence Ratios (SERs), which range from 0 to 0.096. The results show that the varied SERs negligibly influence the time-averaged length of the recirculation zone (about 50 mm off the rear of the strut). However, the low-speed regions in the combustor is increased with SER. High droplet evaporation rates are observable in the downstream of the recirculation zone, and meanwhile continuous evaporation also occurs downstream beyond that due to the local high temperature. The mixing field of the dual-fuel system shows strong inhomogeneity with various compositions of hydrogen/n-heptane/air mixtures in both mixture fraction space and physical space. Moreover, the fraction of heat release rate from hydrogen decreases from 100% to 43.3% due to the increased SERs from 0 to 0.096, and the averaged heat release from hydrogen before blow-off are close, whereas that from n-heptane increases stably. With increased SER, the hydrogen flame base moves upstream towards the strut base, whereas that of n-heptane is lifted off the strut gradually. When SER exceeds some critical value, e.g. 0.096 for the current combustor, the flame blows off, with the two separate reaction zones (upstream hydrogen and downstream n-heptane) fully quenched.
dc.language.isoen
dc.publisherELSEVIER SCI LTD
dc.sourceElements
dc.subjectScience & Technology
dc.subjectTechnology
dc.subjectEnergy & Fuels
dc.subjectEngineering, Chemical
dc.subjectEngineering
dc.subjectn-Heptane spray flame
dc.subjectDual fuel
dc.subjectFlame stabilization
dc.subjectDroplet evaporation
dc.subjectReactant mixing
dc.subjectSupersonic combustion
dc.subjectLARGE-EDDY SIMULATION
dc.subjectCENTRAL SCHEMES
dc.subjectIGNITION
dc.subjectSTABILIZATION
dc.subjectMECHANISM
dc.subjectDYNAMICS
dc.typeArticle
dc.date.updated2020-06-03T02:04:53Z
dc.contributor.departmentMECHANICAL ENGINEERING
dc.description.doi10.1016/j.fuel.2019.116809
dc.description.sourcetitleFUEL
dc.description.volume264
dc.published.statePublished
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