TY - JOUR
T1 - High-speed flamefront imaging in premixed turbulent flames using planar laser-induced fluorescence of the CH C-X band
AU - Carter, Campbell D.
AU - Hammack, Stephen
AU - Lee, Tonghun
N1 - Funding Information:
This work was supported by the U.S. Air Force Research Laboratory, Aerospace Systems Directorate (AFRL/RQ), and the Air Force Office of Scientific Research (AFOSR). University of Illinois contributions were funded through AFOSR grant FA9550-14-1-0343 . In addition, we wish to thank the following people: Dr. Andrei Lipatnikov (Chalmers) for valuable input regarding premixed turbulent flame dynamics; Mr. Aaron Skiba and Mr. Timothy Wabel (University of Michigan) for stimulating discussions regarding flamefront markers; Prof. James Driscoll (University of Michigan) for the loan of the 2D Bunsen burner; and Prof. Adam Steinberg (University of Toronto) for advice in the burner setup.
Publisher Copyright:
© 2016.
PY - 2016/6/1
Y1 - 2016/6/1
N2 - We describe efforts to develop kHz-rate or high-speed planar laser-induced fluorescence (PLIF) of the CH radical for application to premixed flames. The basic approach used here involves excitation and detection of the CH radial via the C2σ+-X2Π (v'=0, v″=0) band, which has transitions in the wavelength range λ≈310-320nm. Transitions in this band are generally stronger than those in the A-X and B-X bands of CH and the radiative lifetimes are shorter too. Thus, the C-X band should have advantages with regard to CH detectability in atmospheric flames, and we show that good CH-PLIF signal-to-noise and signal-to-background ratios can be attained at a 10-kHz interrogation rate and that the spatial resolution (of the CH layer) is reasonably good as well. Of course, strong OH lines, from the A2σ+-X2Π (0,0) and (1,1) bands, lie nearby the CH C-X lines. While this can create some interference in the detection of CH, we demonstrate that OH lines can be avoided, if desired, or excited, if desired. Indeed, easy access to either CH or OH is a substantial benefit of the method outlined herein. Furthermore, we show that simultaneous imaging of CH and OH-using a single laser system and camera-is possible too. We demonstrate the utility of this approach for resolving the flamefront dynamics with 10-kHz measurements in a turbulent, premixed methane-air Bunsen flame: we see intrusion of flame and products into the reactant-zone, which appears to accelerate the consumption of the reactant core, and fingers of flame and reactants that extend into the product-zone and then pinch off and burn out.
AB - We describe efforts to develop kHz-rate or high-speed planar laser-induced fluorescence (PLIF) of the CH radical for application to premixed flames. The basic approach used here involves excitation and detection of the CH radial via the C2σ+-X2Π (v'=0, v″=0) band, which has transitions in the wavelength range λ≈310-320nm. Transitions in this band are generally stronger than those in the A-X and B-X bands of CH and the radiative lifetimes are shorter too. Thus, the C-X band should have advantages with regard to CH detectability in atmospheric flames, and we show that good CH-PLIF signal-to-noise and signal-to-background ratios can be attained at a 10-kHz interrogation rate and that the spatial resolution (of the CH layer) is reasonably good as well. Of course, strong OH lines, from the A2σ+-X2Π (0,0) and (1,1) bands, lie nearby the CH C-X lines. While this can create some interference in the detection of CH, we demonstrate that OH lines can be avoided, if desired, or excited, if desired. Indeed, easy access to either CH or OH is a substantial benefit of the method outlined herein. Furthermore, we show that simultaneous imaging of CH and OH-using a single laser system and camera-is possible too. We demonstrate the utility of this approach for resolving the flamefront dynamics with 10-kHz measurements in a turbulent, premixed methane-air Bunsen flame: we see intrusion of flame and products into the reactant-zone, which appears to accelerate the consumption of the reactant core, and fingers of flame and reactants that extend into the product-zone and then pinch off and burn out.
KW - CH PLIF
KW - KHz diagnostics
KW - Turbulent combustion
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U2 - 10.1016/j.combustflame.2016.03.024
DO - 10.1016/j.combustflame.2016.03.024
M3 - Article
AN - SCOPUS:84964870596
SN - 0010-2180
VL - 168
SP - 66
EP - 74
JO - Combustion and Flame
JF - Combustion and Flame
ER -