Welcome to the new version of CaltechAUTHORS. Login is currently restricted to library staff. If you notice any issues, please email coda@library.caltech.edu
Published January 2012 | Supplemental Material
Journal Article Open

On the formation and early evolution of soot in turbulent nonpremixed flames

Abstract

A 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.

Additional Information

© 2011 The Combustion Institute. Published by Elsevier Inc. Received 24 November 2010; Received in revised form 25 May 2011; Accepted 26 May 2011; Available online 25 June 2011. The 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.

Attached Files

Supplemental Material - mmc1.zip

Files

mmc1.zip
Files (21.1 kB)
Name Size Download all
md5:f66ceceda108dd4b31421b0e54343cb1
21.1 kB Preview Download

Additional details

Created:
August 22, 2023
Modified:
October 24, 2023