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dc.contributor.authorYu, S.
dc.contributor.authorLiu, X.
dc.contributor.authorBai, X. S.
dc.contributor.authorElbaz, Ayman M.
dc.contributor.authorRoberts, William L.
dc.date.accessioned2020-06-15T10:49:34Z
dc.date.available2020-06-15T10:49:34Z
dc.date.issued2020-06-08
dc.date.submitted2019-10-14
dc.identifier.citationYu, S., Liu, X., Bai, X. S., Elbaz, A. M., & Roberts, W. L. (2020). LES/PDF modeling of swirl-stabilized non-premixed methane/air flames with local extinction and re-ignition. Combustion and Flame, 219, 102–119. doi:10.1016/j.combustflame.2020.05.018
dc.identifier.issn1556-2921
dc.identifier.issn0010-2180
dc.identifier.doi10.1016/j.combustflame.2020.05.018
dc.identifier.urihttp://hdl.handle.net/10754/663577
dc.description.abstractTurbulent non-premixed flames with local extinction and re-ignition exhibit multiple combustion modes including ignition waves, diffusion flames, partially premixed flames, and ignition-assisted partially premixed flames. The mechanisms of local extinction and re-ignition are not well understood and numerical modeling of multi-mode combustion is a challenging task. In this work, a specially designed swirl-burner was used to study local extinction and re-ignition of non-premixed turbulent methane/air flames. High speed Particle Image Velocimetry (PIV) and laser induced fluorescence of OH radicals (OH-PLIF) measurements along with Large Eddy Simulation (LES) were carried out to investigate the mechanisms of extinction and re-ignition processes in the burner. LES is based on a transported probability density function model within the framework of Eulerian Stochastic Fields (PDF-ESF). It is found that local extinction occurs when the scalar dissipation rate around the stoichiometric mixture fraction is high. The characteristic time scale for local extinction and re-ignition in the present flames is an order of magnitude longer than the characteristic time scale of diffusion/extinction of laminar flamelets. There are two mechanisms for flame hole re-ignition in the present flames. First, under low degree of local extinction conditions (i.e., for small flame holes surrounded by flames) the flame hole re-ignition is due to the mechanism of turbulent flame folding. Second, under high degree of extinction conditions (i.e., with large regions of extinction and lifted flames), re-ignition of the locally extinguished flame is due to the mechanism of ignition assisted partially premixed flame propagation. The results show that the PDF-ESF model is capable of simulating the quenching and re-ignition process found in the experiments.
dc.description.sponsorshipThe experimental work was supported by competitive research funding from King Abdullah University of Science and Technology (KAUST), Saudi Arabia. The LES work was partly sponsored by Swedish Research Council (VR), and the Swedish Energy Agency (STEM) through the national center for combustion science and technologies (CeCOST) and Lund University Competence Center for Combustion Process (KC-FP). S. Yu and X. Liu were sponsored by China Scholarship Council (CSC). The computations were performed using the computer facilities provided by High Performance Computing Center North (HPC2N), and Center for Parallel Computers (PDC).
dc.publisherElsevier BV
dc.relation.urlhttps://linkinghub.elsevier.com/retrieve/pii/S0010218020302017
dc.rightsNOTICE: this is the author’s version of a work that was accepted for publication in Combustion and Flame. Changes resulting from the publishing process, such as peer review, editing, corrections, structural formatting, and other quality control mechanisms may not be reflected in this document. Changes may have been made to this work since it was submitted for publication. A definitive version was subsequently published in Combustion and Flame, [219, , (2020-06-08)] DOI: 10.1016/j.combustflame.2020.05.018 . © 2020. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/
dc.titleLES/PDF modeling of swirl-stabilized non-premixed methane/air flames with local extinction and re-ignition
dc.typeArticle
dc.contributor.departmentClean Combustion Research Center
dc.contributor.departmentMechanical Engineering Program
dc.contributor.departmentPhysical Science and Engineering (PSE) Division
dc.contributor.departmenthigh-pressure combustion (HPC) Research Group
dc.identifier.journalCombustion and Flame
dc.eprint.versionPost-print
dc.contributor.institutionDivision of Fluid Mechanics, Department of Energy Sciences, Lund University, Lund 22100, Sweden
dc.contributor.institutionCollege of Power and Energy Engineering, Harbin Engineering University, Harbin, Heilongjiang 150001, China
dc.contributor.institutionFaculty of Engineering, Helwan University, Cairo, Egypt
dc.identifier.volume219
dc.identifier.pages102-119
kaust.personElbaz, Ayman M.
kaust.personRoberts, William L.
dc.date.accepted2020-05-24
dc.identifier.eid2-s2.0-85086085878
refterms.dateFOA2020-06-15T12:20:12Z
dc.date.published-online2020-06-08
dc.date.published-print2020-09


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