4.6 Article

Time-averaged probability density functions of soot nanoparticles along the centerline of a piloted turbulent diffusion flame using a scanning mobility particle sizer

Journal

JOURNAL OF AEROSOL SCIENCE
Volume 106, Issue -, Pages 56-67

Publisher

ELSEVIER SCI LTD
DOI: 10.1016/j.jaerosci.2016.10.012

Keywords

Turbulent non-premixed flame; Flame generated aerosols; Flame soot sampling; Soot nanoparticle size distribution; Soot probability density function; Scanning mobility particle sizer (SMPS); Differential mobility analyzer (DMA)

Funding

  1. Clean Combustion Research Center
  2. King Abdullah University of Science and Technology

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In this study, we demonstrate the use of a scanning mobility particle sizer (SMPS) as an effective tool to measure the probability density functions (PDFs) of soot nanoparticles in turbulent flames. Time-averaged soot PDFs necessary for validating existing soot models are reported at intervals of Delta x/D = 5 along the centerline of turbulent, non-premixed, C2H4/N-2 flames. The jet exit Reynolds numbers of the flames investigated were 10,000 and 20,000. A simplified burner geometry based on a published design was chosen to aid modelers. Soot was sampled directly from the flame using a sampling probe with a 0.5-mm diameter orifice and diluted with N-2 by a two-stage dilution process. The overall dilution ratio was not evaluated. An SMPS system was used to analyze soot particle concentrations in the diluted samples. Sampling conditions were optimized over a wide range of dilution ratios to eliminate the effect of agglomeration in the sampling probe. Two differential mobility analyzers (DMAs) with different size ranges were used separately in the SMPS measurements to characterize the entire size range of particles. In both flames, the PDFs were found to be mono-modal in nature near the jet exit. Further downstream, the profiles were flatter with a fall-off at larger particle diameters. The geometric mean of the soot size distributions was less than 10 nm for all cases and increased monotonically with axial distance in both flames.

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