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Extinction and Scattering Properties of Soot Emitted From Buoyant Turbulent Diffusion Flames

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TLDR
In this paper, the extinction and scattering properties at wavelengths of 250-5200 nm were studied for soot emitted from buoyant turbulent diffusion flames in the long residence time regime where soot properties are independent of position in the overfire region and characteristic flame residence times.
Abstract
Extinction and scattering properties at wavelengths of 250-5200 nm were studied for soot emitted from buoyant turbulent diffusion flames in the long residence time regime where soot properties are independent of position in the overfire region and characteristic flame residence times. Flames burning in still air and fueled with gas (acetylene, ethylene, propane, and propylene) and liquid (benzene, toluene, cyclohexane, and n-heptane) hydrocarbon fuels were considered. Measured scattering patterns and ratios of total scattering/absorption cross sections were in good agreement with predictions based on the Rayleigh-Debye-Gans (RDG) scattering approximation in the visible. Measured depolarization ratios were roughly correlated by primary particle size parameter, suggesting potential for completing RDG methodology needed to make soot scattering predictions as well as providing a nonintrusive way to measure primary soot particle diameters. Measurements of dimensionless extinction coefficients were in good agreement with earlier measurements for similar soot populations and were independent of fuel type and wavelength except for reduced values as the near ultraviolet was approached. The ratios of the scattering/absorption refractive index functions were independent of fuel type within experimental uncertainties and were in good agreement with earlier measurements. The refractive index junction for absorption was similarly independent of fuel type but was larger than earlier reflectometry measurements in the infrared. Ratios of total scattering/absorption cross sections were relatively large in the visible and near infrared, with maximum values as large as 0.9 and with values as large as 0.2 at 2000 nm, suggesting greater potential for scattering from soot particles to affect flame radiation properties than previously thought.

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Citations
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Journal ArticleDOI

Laser-induced incandescence : recent trends and current questions

TL;DR: An overview of fundamental experimental and theoretical aspects of soot measurements by laser-induced incandescence (LII) is provided in this paper. But despite the widespread application of LII for soot-concentration and particle-size measurements, there is still a significant lack in fundamental understanding for many of the underlying physical processes.
Journal ArticleDOI

Laser-induced incandescence: Particulate diagnostics for combustion, atmospheric, and industrial applications

TL;DR: A review of laser-induced incandescence (LII) for combustion diagnostics can be found in this paper, where the authors consider two variants of LII, one that is based on pulsed-laser excitation and has been mainly used in combustion diagnostic and emissions measurements, and an alternate approach that relies on continuous-wave lasers and has become increasingly popular for measuring black carbon in environmental applications.
Journal ArticleDOI

Determination of the soot absorption function and thermal accommodation coefficient using low-fluence LII in a laminar coflow ethylene diffusion flame

TL;DR: In this article, the effect of the fractal structure of soot aggregates on the rate of heat loss to the surrounding gas was investigated in the presence of relatively low laser fluences under which soot particles are heated to temperatures below 3500 K.
Journal ArticleDOI

Probing soot formation, chemical and physical evolution, and oxidation: A review of in situ diagnostic techniques and needs

TL;DR: In this article, a review summarizes the chemistry of soot formation and evolution during combustion and describes diagnostic tools that are available to make these measurements and concludes with a brief discussion of needs for new diagnostic tools to probe soot chemistry.
Journal ArticleDOI

A calibration-independent laser-induced incandescence technique for soot measurement by detecting absolute light intensity

TL;DR: A novel LII technique for the determination of soot volume fraction by measuring the absolute incandescence intensity, avoiding the need for ex situ calibration that typically uses a source of particles with known sootVolume fraction.
References
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Book

Absorption and Scattering of Light by Small Particles

TL;DR: In this paper, a Potpourri of Particles is used to describe surface modes in small Particles and the Angular Dependence of Scattering is shown to be a function of the size of the particles.
Journal ArticleDOI

Optical Constants of Soot and Their Application to Heat-Flux Calculations

TL;DR: In this article, the spectral absorption coefficient and the total emissivities of soot suspensions were calculated for the room temperature optiaI.1 and 2.5-1O.
Journal ArticleDOI

Determination of the Wavelength Dependence of Refractive Indices of Flame Soot

TL;DR: In this article, the spectral variation of the optical properties of flame soot particles is determined by combining classical and dynamic light scattering measurements with the Kramers-Kronig relations.
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Radiation heat transfer in combustion systems

TL;DR: In this paper, the authors present a review of the fundamentals of radiation heat transfer and some recent progress in its modeling in combustion systems. But, they do not consider the effects of radiation on the combustion process.
Journal ArticleDOI

Fractal and projected structure properties of soot aggregates

TL;DR: In this paper, the structure of soot aggregates was investigated, emphasizing the fractal properties as well as the relationships between the properties of actual and projected soot images. And the authors found that soot aggregate fractal property is relatively independent of fuel type and flame condition, yielding a fractal dimension of 1.82 with experimental uncertainties of 0.08 and 0.5, respectively.
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