=Paper=
{{Paper
|id=None
|storemode=property
|title=Determination of the dimensionless extinction coefficient for soot generated by a PMMA flame
|pdfUrl=https://ceur-ws.org/Vol-865/Hebert.pdf
|volume=Vol-865
}}
==Determination of the dimensionless extinction coefficient for soot generated by a PMMA flame==
<pdf width="1500px">https://ceur-ws.org/Vol-865/Hebert.pdf</pdf>
<pre>
   Determination of the dimensionless extinction coefficient
            for soot generated by a PMMA flame
   Damien Hebert 1, Alexis Coppalle 1, Jérôme Yon 1 and Martine Talbaut 1
      1
          Laboratoire CORIA - UMR 6614, CNRS - Université et INSA de Rouen, France
                                     hebert@coria.fr

         Experimental soot concentration data in flames are useful for the validation of
soot production and radiation models. Among the experimental methods available in
order to determine soot volume fractions in fluid flows, Laser Induced Incandescence
(LII) is a powerful method allowing to determine local soot volume fractions. Now, this
technic is mature enough to be applied to more and more complex situations
including in the field of fire studies, as in the present study. LII has been applied to
the determination of soot volume fraction fields in the flame of a vertical PMMA slab.
Indeed, during solid material combustion, the fuel pyrolysis is a key phenomenon,
which depends on the heat transfer between the flame and the unburnt material [1].
So, as a source of radiation, soot particles play an important role in the solid material
combustion.
         An important step of the LII signal analysis is the calibration, in order to
determine the relationship between the LII signal and the soot volume fraction [2].
The most-used approach for calibration consists in measuring the light extinction
coefficient Kext, which depends on soot volume fraction fv. Kext is also a function of
soot particle morphology and of the optical index of the soot matter, which varies with
the wavelength. But much of the optical index or Kext data for soot have been
determined from measurements in gaseous or liquid fueled flames but few for the
solid combustion. Additionally, Kext has been usually determined ex-situ for soot
samples at ambient temperature [3]. Therefore one can wonder if the soot optical
properties at standard or flame temperatures can be considered similar. The present
work focuses on this question.
         In this context, the spectral value of Kext has been measured by using in-situ
extinction measurements with a white laser beam (Leukos) crossing the flat flame of
a PMMA slab. With the same experimental setup, Kext is also determined in a
gaseous fueled flame generated by a bronze porous burner and fed with a mixing of
methane and ethylene. So the determined Kext coefficients are relevant of the soot
optical properties at high temperatures. In order to observe the influence of the soot
temperature on the spectral variation of Kext, it has been also determined by ex-situ
measurements after sampling of soot in the flame [4]. This sampling has allowed
additional measurements, the agglomerate soot particle size using a Scanning
Mobility Particle Sizer (SMPS) and the mass concentration with a Tapered Element
Oscillating Microbalance (TEOM).
         The experimental results are analyzed to compare the spectral variations of
Kext in the 400-1100 nm range. Finally, different evaluations of the dimensionless
extinction coefficient Ke=Kext/fv are proposed corresponding to soot generated by
gaseous or solid combustion at standard or flame temperatures. A quantitative
comparison with the values found in the literature is presented.

[1] A.C. Fernandez-Pello and T. Hirano, Combust. Sci. Technol. 32 (1983) 1-31.
[2] C. Schulz et al, Appl. Phys. B 83 (2006) 333-354.
[3] G.W. Mulholland and M.Y. Choi, Symp. Int. Combust. 27 (1998) 1515.
[4] J. Yon et al, Appl. Phys. B 104 (2011) 253-271.




               5th international workshop on Laser-Induced Incandescence
                May 9-11, 2012, Palais des Congrès, Le Touquet, France

</pre>