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Effect of aggregation on the absorption cross-section of fractal soot aggregates and its impact on LII modelling

 
 
Affiliation:
National Research Council Canada (NRC-CNRC); NRC Institute for Chemical Process and Environmental Technology
Language:
English
Type:
Article
Published in:
Journal of Quantitative Spectroscopy and Radiative Transfer
Date:
2010
Pages :
302-308
NRCC #:
52044
NPArC #:
15195100
Keywords:
Fractal soot aggregates; Absorption cross-section; Laser-induced incandescence
Program(s):
Environment Monitoring Technologies; Technologies de surveillance de l'environnement
Project(s):
LII - Nanoparticle Diagnostics and Characterization; LII - Diagnostic et caractérisation des nanoparticules
Group(s):
Environment Monitoring Technologies Program; Programme des technologies de surveillance de l'environnement
Abstract:
This study concerns the effect of particle aggregation on laser heating rate of soot aggregates in laser-induced incandescence. Three aggregate absorption models were investigated: the Rayleigh–Debye–Gans approximation, the electrostatics approxima- tion, and the numerically exact generalized multi-sphere Mie-solution method. Fractal aggregates containing 5–893 primary particles of 30nm in diameter were generated numerically using a combined particle cluster and cluster-cluster aggregation algorithm with specific fractal parameters typical of soot. The primary particle size parameters considered are 0.089, 0.177, and 0.354. The Rayleigh–Debye–Gans approximation neglects the effect of particle aggregation on absorption; so it underestimates the aggregate absorption cross-section area by approximately 10%, depending on the aggregate size and primary particle size parameter. The electrostatics approximation is somewhat better than the Rayleigh–Debye–Gans approximation, but cannot account for the effect of primary particle size parameter. The aggregate absorption submodel affects the calculated soot temperature in laser-induced incandescence mainly in the low laser fluence regime. At high laser fluences, the effect diminishes due to the enhanced importance of soot sublimation cooling and neglect of aggregation effect in the sublimation in the present numerical model of laser-induced incandescence.
 
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