Morphology and mobility diameter of carbonaceous aerosols during agglomeration and surface growth

Georgios A. Kelesidis, Eirini Goudeli, Sotiris E. Pratsinis

Research output: Contribution to journalArticlepeer-review

20 Scopus citations

Abstract

Agglomeration and surface growth of fractal-like carbonaceous aerosols in the absence of oxidation and condensation of volatiles are investigated by Discrete Element Modeling (DEM) from the free molecular to transition regime, accounting for primary particle polydispersity and chemical bonding (aggregation). That way, carbon black or soot formation is elucidated in plasma reactors, quenched flames and combustion engines running at high exhaust gas recirculation where oxidation of carbon is limited or non-existent. During nascent soot formation polydisperse spheres and aggregates are formed, attaining an asymptotic geometric standard deviation of 1.2 ± 0.01, in agreement with experiments in premixed, diffusion flames and wood combustion. When surface growth stops, mature soot grows by agglomeration of these polydisperse spheres and aggregates before oxidation and condensation take over. The evolution from nascent to mature soot morphology quantified by its fractal dimension, Df, and mass-mobility exponent, Dfm, is in good agreement with measurements in premixed, diffusion flames and the Cast soot generator. The mobility diameter, dm, can be related to the average number of primary particles per agglomerate by nva = (dm/dva)0.45 and the relative effective density of soot by ρeffs = (dm/dva)−0.78, where dva is the primary particle diameter and ρs the soot bulk density.

Original languageEnglish (US)
Pages (from-to)527-535
Number of pages9
JournalCarbon
Volume121
DOIs
StatePublished - Sep 2017

Bibliographical note

Funding Information:
The research leading to these results has received funding from the Swiss National Science Foundation (grant no. 200021_149144) and ETH Zurich (grant no. ETH-08 14-2).

Keywords

  • Effective density
  • Fractal dimension
  • Mass-mobility exponent
  • Mobility diameter
  • Soot morphology

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