Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/116297
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dc.contributorDepartment of Mechanical Engineeringen_US
dc.creatorRay, Sen_US
dc.creatorCheng, Sen_US
dc.date.accessioned2025-12-15T06:18:41Z-
dc.date.available2025-12-15T06:18:41Z-
dc.identifier.issn1070-6631en_US
dc.identifier.urihttp://hdl.handle.net/10397/116297-
dc.language.isoenen_US
dc.publisherAIP Publishing LLCen_US
dc.rights© 2025 Author(s). Published under an exclusive license by AIP Publishing.en_US
dc.rightsThis is the accepted version of the publication.en_US
dc.rightsThis article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. This article appeared in Saroj Ray, Song Cheng; Microexplosion in burning emulsified fuel droplets. Physics of Fluids 1 August 2025; 37 (8): 082134 and may be found at https://doi.org/10.1063/5.0287392.en_US
dc.titleMicroexplosion in burning emulsified fuel dropletsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume37en_US
dc.identifier.issue8en_US
dc.identifier.doi10.1063/5.0287392en_US
dcterms.abstractThis paper presents an analytical model for simulating microexplosions in burning emulsified fuel droplets. A key feature of the proposed model is its ability to capture bubble growth within a droplet, which triggers microexplosions, while also incorporating the effects of droplet combustion. The model offers a comprehensive formulation for a single bubble inside a burning droplet, accounting for bubble dynamics, heat transfer, phase change, and combustion processes. The methodology outlining the mathematical framework, governing equations, and underlying assumptions are presented. The model is applied specifically to n-dodecane/water emulsion droplets, and the results are analyzed in detail and validated against experimental data from previous studies. The evolution of the bubble radius reveals two distinct growth stages: an initial thermally controlled phase followed by an inertially controlled phase. Droplet growth also proceeds in two stages—initially independent of bubble growth, and later becoming interdependent. Notably, the microexplosion delay time decreases gradually with increasing initial bubble radius but increases sharply with a larger initial droplet radius. The developed analytical model has the potential for simulating spray combustion of water-emulsified fuels with significantly reduced computational cost while maintaining sufficient fidelity.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationPhysics of fluids, Aug. 2025, v. 37, no. 8, 082134en_US
dcterms.isPartOfPhysics of fluidsen_US
dcterms.issued2025-08-
dc.identifier.scopus2-s2.0-105013687010-
dc.identifier.eissn1089-7666en_US
dc.identifier.artn082134en_US
dc.description.validate202512 bcchen_US
dc.description.oaAccepted Manuscripten_US
dc.identifier.SubFormIDG000483/2025-09-
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextThis work is supported by Research seed fund at NIT Rourkela, India, and by the Research Grants Council of the Hong Kong Special Administrative Region, China, under No. 25104223 for the ECS project funded in 2023/24 Exercise.en_US
dc.description.pubStatusPublisheden_US
dc.date.embargo2026-08-31 (Version of Record)en_US
dc.description.oaCategoryVoR alloweden_US
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