Opposed jet flames of lean or rich premixed propane-air reactants versus hot products

Several opposed jet flames, produced by a lean H₂-air jet opposing a rich or lean C₃H₈-air jet, are investigated. Spontaneous Raman spectroscopy is used for major species concentration and temperature measurements along the opposed jet centerline. The hot products of the H₂-air flame simulate the burnt gases of strong-burning near-stoichiometric reactants as they impinge upon a weak-burning lean or rich hydrocarbon-fueled reactant mix, a situation encountered in stratified charge operation of direct injection spark ignition engines. In addition the H₂-air flame hot products facilitate experimental data interpretation through the absence of carbon-bearing species. Good agreement between numerical and experimental data are obtained for a rich (equivalence ratio, φ = 1.25) C₃H₈-air jet versus a lean (φ = 0.4) H₂-air jet. Two lean C₃H₈-air jets (φ = 0.64 or 0.60), versus the φ = 0.4 H₂-air jet, are also investigated. For both of these flames, the amount of CO₂ production strongly depends upon φ, with the φ = 0.64 flame having a peak CO₂ mole fraction an order of magnitude higher than for the φ = 0.60 flame, and the C₃H₈ flames burning either as a normal flame (high CO₂) or as a “negative flame speed” flame producing little CO₂ and then only through diffusion of C₃H₈ into the hot products jet. The numerically predicted and experimental CO₂ profiles agree well for the positive flame speed flame, but the large discrepancy between predicted and measured peak CO₂ in the negative flame speed flame suggests modeling improvements are needed for this type of flame.