Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Lee, SR | - |
dc.contributor.author | Kim, JS | - |
dc.date.accessioned | 2024-01-21T14:14:29Z | - |
dc.date.available | 2024-01-21T14:14:29Z | - |
dc.date.created | 2021-09-05 | - |
dc.date.issued | 2000-03 | - |
dc.identifier.issn | 1364-7830 | - |
dc.identifier.uri | https://pubs.kist.re.kr/handle/201004/141548 | - |
dc.description.abstract | The nonlinear dynamics of striped diffusion flames, formed in the two-dimensional counterflow field by the diffusional-thermal instability with Lewis numbers sufficiently less than unity, is investigated numerically by examining the nonlinear two-dimensional transient flame-structure solutions bifurcating from the one-dimensional steady solution by various initial perturbations. The Lewis numbers for the fuel and oxidizer are assumed to be identical and an overall single-step Arrhenius-type chemical reaction rate is employed as the chemistry model. Attention is focused on two nonlinear phenomena, namely the development of the two-dimensional flame-stripe structure and the extension of the flammability limit beyond the static extinction condition of a one-dimensional flame. A time-dependent solution, carried out for a Damkohler number slightly above the static extinction Damkohler number, exhibited the developmental procedure of flame stripes with the most unstable wavelength from a long-wave initial perturbation with a small amplitude. In contrast to the chaotic cellular premixed-flame structures predicted from numerical integration of the Kuramoto-Sivashinsky equation, the stripe structure in diffusion flames is found to be stationary consequently leading to the conclusion that the nonlinear term in the corresponding nonlinear bifurcation equation would be a simple cubic term. Two-dimensional flame-stripe solutions are also found to be able to survive Damkohler numbers significantly below the static extinction Damkohler number of the one-dimensional flame structure. Extension of the flammability is found to be greatest if the imposed initial perturbation possesses the wavenumber of the fastest growing mode. | - |
dc.language | English | - |
dc.publisher | IOP PUBLISHING LTD | - |
dc.subject | NON-LINEAR ANALYSIS | - |
dc.subject | HYDRODYNAMIC INSTABILITY | - |
dc.subject | PATTERN-FORMATION | - |
dc.subject | LAMINAR FLAMES | - |
dc.subject | LEWIS NUMBERS | - |
dc.title | Nonlinear dynamic characteristics of flame stripes formed in strained diffusion flames by diffusional-thermal instability | - |
dc.type | Article | - |
dc.identifier.doi | 10.1088/1364-7830/4/1/302 | - |
dc.description.journalClass | 1 | - |
dc.identifier.bibliographicCitation | COMBUSTION THEORY AND MODELLING, v.4, no.1, pp.29 - 46 | - |
dc.citation.title | COMBUSTION THEORY AND MODELLING | - |
dc.citation.volume | 4 | - |
dc.citation.number | 1 | - |
dc.citation.startPage | 29 | - |
dc.citation.endPage | 46 | - |
dc.description.journalRegisteredClass | scie | - |
dc.description.journalRegisteredClass | scopus | - |
dc.identifier.wosid | 000087098700002 | - |
dc.identifier.scopusid | 2-s2.0-0033994887 | - |
dc.relation.journalWebOfScienceCategory | Thermodynamics | - |
dc.relation.journalWebOfScienceCategory | Energy & Fuels | - |
dc.relation.journalWebOfScienceCategory | Engineering, Chemical | - |
dc.relation.journalWebOfScienceCategory | Mathematics, Interdisciplinary Applications | - |
dc.relation.journalResearchArea | Thermodynamics | - |
dc.relation.journalResearchArea | Energy & Fuels | - |
dc.relation.journalResearchArea | Engineering | - |
dc.relation.journalResearchArea | Mathematics | - |
dc.type.docType | Article | - |
dc.subject.keywordPlus | NON-LINEAR ANALYSIS | - |
dc.subject.keywordPlus | HYDRODYNAMIC INSTABILITY | - |
dc.subject.keywordPlus | PATTERN-FORMATION | - |
dc.subject.keywordPlus | LAMINAR FLAMES | - |
dc.subject.keywordPlus | LEWIS NUMBERS | - |
dc.subject.keywordAuthor | flame instability | - |
dc.subject.keywordAuthor | extinction | - |
dc.subject.keywordAuthor | diffusional-thermal instability | - |
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