Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/78695
Citations
Scopus Web of Science® Altmetric
?
?
Type: Journal article
Title: Experimental and computational study of soot evolution in a turbulent nonpremixed bluff body ethylene flame
Author: Mueller, M.
Chan, Q.
Qamar, N.
Dally, B.
Pitsch, H.
Alwahabi, Z.
Nathan, G.
Citation: Combustion and Flame, 2013; 160(7):1298-1309
Publisher: Elsevier Science Inc
Issue Date: 2013
ISSN: 0010-2180
1556-2921
Statement of
Responsibility: 
Michael E. Mueller, Qing N. Chan, Nader H. Qamar, Bassam B. Dally, Heinz Pitsch, Zeyad T. Alwahabi, Graham J. Nathan
Abstract: A turbulent nonpremixed bluff body ethylene flame is studied both experimentally and computationally. Experimentally, the soot volume fraction is measured using laser-induced incandescence (LII). Three distinct regions are observed in the flame: a low-strain recirculation zone, a downstream jet-like region, and a high-strain neck region connecting these two regions. The maximum soot volume fraction is found in the recirculation zone, but most of the soot volume is contained in the larger jet-like region further downstream. In the neck region between these two zones, soot cannot form due to large strain rates, and the small amounts of soot in this region indicate that soot rarely escapes the recirculation zone before being oxidized. The recirculation zone is characterized by a low soot intermittency, in contrast to the downstream jet-like region and previously investigated jet flames in which the soot intermittency is high. Large Eddy Simulation (LES) is used to further investigate this distinctly different evolution of soot in the recirculation zone. The LES model is found to predict the soot volume fraction profiles quite accurately, albeit with significant sensitivity to the inflow profiles of the fuel jet and air coflow. Soot is formed near the inner shear layer between the fuel jet and recirculation zone where the mixture fraction is sufficiently large to support Polycyclic Aromatic Hydrocarbon (PAH) formation. A portion of this soot is entrained into the interior of the recirculation zone where the soot growth rates are relatively low, despite the rich mixture fraction in this region. The circulation vortex then transports the soot from the interior of the recirculation zone toward less rich mixture fractions near the flame, which is situated in the outer shear layer between the air coflow and the recirculation zone. Here, the majority of soot growth occurs due to surface growth, that is, mass addition due to surface reactions with acetylene. The dominance of acetylene-based surface growth in the recirculation zone contrasts findings in previous simulations of turbulent jet flames that do not exhibit a recirculation zone, in which nucleation and PAH condensation were found to overwhelm acetylene-based surface growth. © 2013 The Combustion Institute.
Keywords: Soot
Laser-induced incandescence
Large Eddy Simulation
Bluff body flame
Turbulent nonpremixed flame
Rights: Copyright © 2013 The Combustion Institute.
DOI: 10.1016/j.combustflame.2013.02.010
Published version: http://dx.doi.org/10.1016/j.combustflame.2013.02.010
Appears in Collections:Aurora harvest 4
Chemical Engineering publications
Environment Institute publications

Files in This Item:
There are no files associated with this item.


Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.