Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/111640
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dc.contributorDepartment of Aeronautical and Aviation Engineeringen_US
dc.creatorLi, Xen_US
dc.creatorHao, Jen_US
dc.creatorFan, Een_US
dc.creatorUy, KCKen_US
dc.creatorShao, Xen_US
dc.creatorWen, CYen_US
dc.date.accessioned2025-03-04T06:43:36Z-
dc.date.available2025-03-04T06:43:36Z-
dc.identifier.issn0360-3199en_US
dc.identifier.urihttp://hdl.handle.net/10397/111640-
dc.language.isoenen_US
dc.publisherPergamon Pressen_US
dc.rights© 2025 The Authors. Published by Elsevier Ltd on behalf of Hydrogen Energy Publications LLC.This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/).en_US
dc.rightsThe following publication Li, X., Hao, J., Fan, E., Uy, K. C. K., Shao, X., & Wen, C. Y. (2025). Evolution of shock-induced reactive and inert double-layer gas cylinders. International Journal of Hydrogen Energy, 109, 1064-1080 is available at https://doi.org/10.1016/j.ijhydene.2025.02.175.en_US
dc.titleEvolution of shock-induced reactive and inert double-layer gas cylindersen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1064en_US
dc.identifier.epage1080en_US
dc.identifier.volume109en_US
dc.identifier.doi10.1016/j.ijhydene.2025.02.175en_US
dcterms.abstractThe evolution and mixing of shock-induced reactive and inert double-layer gas cylinders are numerically investigated, with inner-to-outer radius ratios (λ) ranging from 0.25 to 0.75. In reactive cases, a hot spot forms near the downstream interface of the outer cylinder due to high pressure and temperature from the triple point. When λ increases to 0.75, a second hot spot appears near the upstream interface of the inner cylinder. The distribution of pressure, temperature, and hydrogen mass fraction at the reaction front indicates that deflagration-to-detonation occurs after the generation of the first hot spot. Following the second hot spot, a detonation wave propagates upstream towards the outer interface. Intense heat release following ignition causes an expansion in the outer diameter and the area of the gas ring, while compressing the inner diameter and inner gas area. Detonation results in a more rapid increase in combustion completeness compared to deflagration. Regarding vorticity and mixing fraction, the magnitude of net vorticity decreases, and its rate of decrease slows after ignition as the radius ratio increases. Additionally, the mixing fraction between the mixture in the gas ring and the ambient gas increases with increasing radius ratios in both reactive and inert gas cylinders but remains lower in reactive cylinders compared to inert ones after ignition.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationInternational journal of hydrogen energy, 14 Mar. 2025, v. 109, p. 1064-1080en_US
dcterms.isPartOfInternational journal of hydrogen energyen_US
dcterms.issued2025-03-14-
dc.identifier.scopus2-s2.0-85217758791-
dc.identifier.eissn1879-3487en_US
dc.description.validate202503 bchyen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_TA-
dc.description.fundingSourceRGCen_US
dc.description.pubStatusPublisheden_US
dc.description.TAElsevier (2025)en_US
dc.description.oaCategoryTAen_US
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