Abstract
Detailed measurements of reactive and passive scalars in axisymmetric bluff-body flames of CH
4/H
2, CH
4/air, and CO/H
2 have been reported in the past
[1] and have been used in several studies directed at developing and validating turbulent combustion models
[2–5]. Comparisons of measured and modeled results for flames with CH
4/H
2 as fuel have shown significant disagreement in the mass fractions of CO, with the Raman scattering measurements of [CO] being much higher than the modeling calculations. Previously published data
[1] were collected using the Raman scattering technique for all major species including CO. Raman scattering measurements of [CO] in methane flames suffer from laser-excited interference from higher hydrocarbons formed on the fuel-rich side of the reaction zone. It is well established
[6–8] that measurements of [CO] based on two-photon laser-induced fluorescence (TPLIF) can provide much better accuracy than those based on Raman scattering in methane and natural gas flames.Keywords: Bluff body; CO; LIF; Raman; Flame