TY - JOUR
T1 - Measurements of Pressure Effects on PAH Distribution and 2D Soot Volume Fraction Diagnostics in a Laminar Non-premixed Coflow Flame
AU - Bennett, Anthony
AU - Amin, Hafiz M.F.
AU - Cenker, Emre
AU - Roberts, William L.
PY - 2018/10/18
Y1 - 2018/10/18
N2 - The soot formation process has been investigated at pressures up to 16
bar using a non-premixed laminar coflow flame with nitrogen-diluted
ethylene. 2D diffuse line-of-sight attenuation (2D LOSA) and planar
laser-induced incandescence (PLII) were used to measure soot volume
fraction (SVF). The peak SVF increased exponentially with increasing
pressure, and the spatial distribution of soot volume fraction changed
substantially. At pressures below 6 bar, the two techniques agreed well.
At pressures above 6 bar, the techniques began to disagree, with 2D
LOSA showing higher peak SVF values at a location lower in the wings of
the flame compared to PLII. Errors in the LOSA measurements due to the
molecular absorption of PAHs were assessed by performing measurements
with bandpass filters centered at 435 nm and at 647 nm. Furthermore, the
evolution of polycyclic aromatic hydrocarbons (PAH) in the flame was
studied using planar laser-induced fluorescence (PLIF) with the
excitation laser set at 282.85 nm and compared to LOSA measurements.
Fluorescence signals were captured using bandpass filters (350, 400,
450, and 510 nm) corresponding to increasing PAH size. The peak
concentration of PAHs moved closer to the burner nozzle as pressure
increased. Absorption by PAH was unable to explain discrepancies between
LOSA measurements and PLII measurements. Using the Rayleigh–Debye–Gans
approximation for polydisperse fractal aggregates (RDG-PFA), the
differences between LOSA and PLII measurements were analyzed, and it was
found that LOSA is more sensitive to the soot primary particle diameter
due to changes in the scattering-to-absorption ratio (ρsa). The effect of gate duration on SVF imaging with PLII is also reported.
AB - The soot formation process has been investigated at pressures up to 16
bar using a non-premixed laminar coflow flame with nitrogen-diluted
ethylene. 2D diffuse line-of-sight attenuation (2D LOSA) and planar
laser-induced incandescence (PLII) were used to measure soot volume
fraction (SVF). The peak SVF increased exponentially with increasing
pressure, and the spatial distribution of soot volume fraction changed
substantially. At pressures below 6 bar, the two techniques agreed well.
At pressures above 6 bar, the techniques began to disagree, with 2D
LOSA showing higher peak SVF values at a location lower in the wings of
the flame compared to PLII. Errors in the LOSA measurements due to the
molecular absorption of PAHs were assessed by performing measurements
with bandpass filters centered at 435 nm and at 647 nm. Furthermore, the
evolution of polycyclic aromatic hydrocarbons (PAH) in the flame was
studied using planar laser-induced fluorescence (PLIF) with the
excitation laser set at 282.85 nm and compared to LOSA measurements.
Fluorescence signals were captured using bandpass filters (350, 400,
450, and 510 nm) corresponding to increasing PAH size. The peak
concentration of PAHs moved closer to the burner nozzle as pressure
increased. Absorption by PAH was unable to explain discrepancies between
LOSA measurements and PLII measurements. Using the Rayleigh–Debye–Gans
approximation for polydisperse fractal aggregates (RDG-PFA), the
differences between LOSA and PLII measurements were analyzed, and it was
found that LOSA is more sensitive to the soot primary particle diameter
due to changes in the scattering-to-absorption ratio (ρsa). The effect of gate duration on SVF imaging with PLII is also reported.
UR - http://www.scopus.com/inward/record.url?scp=85053931960&partnerID=8YFLogxK
U2 - 10.1021/acs.energyfuels.8b02179
DO - 10.1021/acs.energyfuels.8b02179
M3 - Article
AN - SCOPUS:85053931960
SN - 0887-0624
VL - 32
SP - 10974
EP - 10983
JO - Energy and Fuels
JF - Energy and Fuels
IS - 10
ER -