Optical measurement of volume fraction and organic mass fraction of ultra-fine soot particles emitted from inverse diffusion flames

Fuel ◽  
2017 ◽  
Vol 210 ◽  
pp. 455-462 ◽  
Author(s):  
Sangchul Lim ◽  
Taekook Ahn ◽  
Seunghoon Lee ◽  
Sunho Park
Fuel ◽  
2012 ◽  
Vol 102 ◽  
pp. 199-207 ◽  
Author(s):  
Yongjin Jung ◽  
Kwang Chul Oh ◽  
Choongsik Bae ◽  
Hyun Dong Shin

1997 ◽  
Vol 110 (3) ◽  
pp. 405-408 ◽  
Author(s):  
Erin M. Clausing ◽  
Dwight W. Senser ◽  
Normand M. Laurendeau

2013 ◽  
Vol 20 (11) ◽  
pp. 1671-1681 ◽  
Author(s):  
Yat Sze Choy ◽  
Hai Sheng Zhen ◽  
Chun Wah Leung ◽  
Chun Shun Cheung ◽  
Randolph Chi Kin Leung

1983 ◽  
Vol 105 (1) ◽  
pp. 159-165 ◽  
Author(s):  
R. A. Beier ◽  
P. J. Pagni

A multiwavelength laser transmission technique is used to determine soot volume fraction fields and aproximate particle size distributions in a forced flow combusting boundary layer. Measurements are made in diffusion flames of polymethylmethacrylate (PMMA) and five liquid hydrocarbon fuels (n-heptane, iso-octane, cyclohexane, cyclohexene, and toluene) with ambient oxygen mass fractions in the range of 0.23 ≲ Y0∞ ≲ 0.50. Soot is observed in a region between the pyrolyzing fuel surface and the flame zone. Soot volume fraction increases monotonically with Y0∞, e.g., n-heptane and PMMA are similar with soot volume fractions, fν, ranging from fν ∼ 5 × 10−7 at Y0∞ = 0.23 to fν ∼ 5 × 10−6 at Y0∞ = 0.50. For an oxygen mass fraction the same as air, Y0∞ = 0.23, soot volume fractions are approximately the same as values previously reported in pool fires and a free combusting boundary layer. However, the shape of the fν profile changes with more soot near the flame in forced flow than in free flow due to the different y-velocity fields in these two systems. For all fuels tested, a most probable particle radius is between 20 nm and 80 nm, and does not appear to change substantially with location, fuel, or oxygen mass fraction.


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