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dc.contributor.authorVashishtha, Ashish
dc.contributor.authorKore, Rushikesh
dc.contributor.authorPalateerdham, Sasi Kiran
dc.contributor.authorIngenito, Antonella
dc.date.accessioned2024-05-16T15:15:23Z
dc.date.available2024-05-16T15:15:23Z
dc.date.copyright2024-04
dc.date.issued2024-04-14
dc.identifier.citationVashishtha, A., Kore, R., Palateerdham, S.K. and Ingenito, A. (2024). Numerical study of hydrogen Injection in crossflow to initiate oblique detonation wave. In proceedings HiSST: 3rd International Conference on High-Speed Vehicle Science Technology.en_US
dc.identifier.urihttps://research.thea.ie/handle/20.500.12065/4814
dc.description.abstractWith the motivation of operating scramjet in shock induced combustion ramjet (shcramjet) or oblique detonation wave mode, the current study aims to develop strategies for non-premixed oblique detonation wave configuration using numerical simulations. The unsteady two-dimensional Reynolds Averaged Navier-Stokes with reactive multi-species equations are solved using adaptive grid refinement and robust SAGE solver on CONVERGE-CFD platform with detailed chemical kinetics. The sonic hydrogen injection cases (ϕ = 0.5) into incoming air flow at Mach 7 with pressure of 40 kPa and temperature of 300 K are simulated for 2 ms duration. The computational domain consists of finite length wedge (100 mm, θw = 26◦ as well as hydrogen injection tube upstream of wedge starting point, to obtain non-premixed oblique detonation wave. The unsteady detonation wave patterns are obtained for angle of injection (AOI) 15◦ with injector location at (Dj=) 30 mm from wedge tip. It is found that various flow features, such as jet-shock, shear layer and hot burnt zone near the wedge wall affect the lifted detonation wave starting at the interaction point of shear layer and hot burnt zone. The detonation wave momentarily transition to deflagration flame and re-establish itself as detonation wave multiple times. The angle of injection (AOI) and injector locations are varied to obtain various patterns of unsteady non-premixed oblique detonation wave and it was found that AOIs below or close to wedge angle lead to formation of unsteady oblique detonation wave, while AOIs higher than the wedge angle lead to formation of stable stretched deflagration flame. Injection location very close to wedge starting point leads to multi-cycle detonation to deflagration transitions and deflagration to detonation transitions. The overall thermal and combustion efficiencies are alsoen_US
dc.formatapplication/pdfen_US
dc.language.isoengen_US
dc.publisherCEASen_US
dc.relation.ispartof3rd International Conference on High-Speed Vehicle Science Technologyen_US
dc.rightsAttribution-NonCommercial-NoDerivs 3.0 United States*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/us/*
dc.subjectNumerical Simulationsen_US
dc.subjectJet Injectionen_US
dc.subjectShock induced Combustionen_US
dc.subjectDetonationen_US
dc.subjectNon-premixed combustionen_US
dc.titleNumerical study of hydrogen injection to initiate oblique detonation waveen_US
dc.typeinfo:eu-repo/semantics/conferenceObjecten_US
dc.conference.date2024-04-14
dc.conference.hostConference of European Aerospace Societiesen_US
dc.conference.locationBusan, Koreaen_US
dc.contributor.affiliationSouth East Technological University: Carlow Campusen_US
dc.description.peerreviewyesen_US
dc.identifier.doi10.13009/EUCASS2023-866en_US
dc.identifier.orcidhttps://orcid.org/0000-0002-8385-3740en_US
dc.rights.accessrightsinfo:eu-repo/semantics/openAccessen_US
dc.subject.departmentEngCOREen_US
dc.type.versioninfo:eu-repo/semantics/publishedVersionen_US
cr.approval.ethical


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Attribution-NonCommercial-NoDerivs 3.0 United States
Except where otherwise noted, this item's license is described as Attribution-NonCommercial-NoDerivs 3.0 United States