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dc.contributor.authorBisetti, Fabrizio
dc.contributor.authorBlanquart, Guillaume
dc.contributor.authorMüeller, Michael E.
dc.contributor.authorPitsch, Heinz G.
dc.date.accessioned2015-08-03T09:43:28Z
dc.date.available2015-08-03T09:43:28Z
dc.date.issued2012-01
dc.identifier.citationBisetti, F., Blanquart, G., Mueller, M. E., & Pitsch, H. (2012). On the formation and early evolution of soot in turbulent nonpremixed flames. Combustion and Flame, 159(1), 317–335. doi:10.1016/j.combustflame.2011.05.021
dc.identifier.issn00102180
dc.identifier.doi10.1016/j.combustflame.2011.05.021
dc.identifier.urihttp://hdl.handle.net/10754/562043
dc.description.abstractA Direct Numerical Simulation (DNS) of soot formation in an n-heptane/air turbulent nonpremixed flame has been performed to investigate unsteady strain effects on soot growth and transport. For the first time in a DNS of turbulent combustion, Polycyclic Aromatic Hydrocarbons (PAH) are included via a validated, reduced chemical mechanism. A novel statistical representation of soot aggregates based on the Hybrid Method of Moments is used [M.E. Mueller, G. Blanquart, H. Pitsch, Combust. Flame 156 (2009) 1143-1155], which allows for an accurate state-of-the-art description of soot number density, volume fraction, and morphology of the aggregates. In agreement with previous experimental studies in laminar flames, Damköhler number effects are found to be significant for PAH. Soot nucleation and growth from PAH are locally inhibited by high scalar dissipation rate, thus providing a possible explanation for the experimentally observed reduction of soot yields at increasing levels of mixing in turbulent sooting flames. Furthermore, our data indicate that soot growth models that rely on smaller hydrocarbon species such as acetylene as a proxy for large PAH molecules ignore or misrepresent the effects of turbulent mixing and hydrodynamic strain on soot formation due to differences in the species Damköhler number. Upon formation on the rich side of the flame, soot is displaced relative to curved mixture fraction iso-surfaces due to differential diffusion effects between soot and the gas-phase. Soot traveling towards the flame is oxidized, and aggregates displaced away from the flame grow primarily by condensation of PAH on the particle surface. In contrast to previous DNS studies based on simplified soot and chemistry models, surface reactions are found to contribute barely to the growth of soot, for nucleation and condensation processes occurring in the fuel stream are responsible for the most of soot mass generation. Furthermore, the morphology of the soot aggregates is found to depend on the location of soot in mixture fraction space. Aggregates having the largest primary particles populate the region closest to the location of peak soot growth. On the contrary, the aggregates with the largest number of primary particles are located much further into the fuel stream. © 2011 The Combustion Institute.
dc.description.sponsorshipThe authors gratefully acknowledge funding from the Strategic Environmental Research and Development Program (SERDP) and the National Aeronautics and Space Administration (NASA). This research was supported in part by the National Science Foundation (NSF) through TeraGrid resources provided by the Texas Advanced Computing Center (TACC) under Grant No. TG-CTS090021. M.E.M. gratefully acknowledges support of the National Defense Science and Engineering Graduate (NDSEG) fellowship program. The authors would like to thank Dr. Pepiot-Desjardins for her help in reducing the chemical mechanism.
dc.publisherElsevier BV
dc.subjectDirect numerical simulation
dc.subjectN-heptane
dc.subjectParticulate morphology
dc.subjectPolycyclic aromatic hydrocarbons
dc.subjectSoot
dc.subjectTurbulent nonpremixed combustion
dc.titleOn the formation and early evolution of soot in turbulent nonpremixed flames
dc.typeArticle
dc.contributor.departmentClean Combustion Research Center
dc.contributor.departmentMechanical Engineering Program
dc.contributor.departmentPhysical Science and Engineering (PSE) Division
dc.contributor.departmentReactive Flow Modeling Laboratory (RFML)
dc.identifier.journalCombustion and Flame
dc.contributor.institutionDepartment of Mechanical Engineering, California Institute of Technology, Pasadena, CA 91125, United States
dc.contributor.institutionDepartment of Mechanical Engineering, Stanford University, Stanford, CA 94305, United States
dc.contributor.institutionInstitut für Technische Verbrennung, RWTH Aachen University, 52056 Aachen, Germany
kaust.personBisetti, Fabrizio


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