Tg. Kreutz et Ck. Law, IGNITION IN NONPREMIXED COUNTERFLOWING HYDROGEN VERSUS HEATED AIR - COMPUTATIONAL STUDY WITH DETAILED CHEMISTRY, Combustion and flame, 104(1-2), 1996, pp. 157-175
Forced ignition in counterflowing jets of N-2-diluted H-2 versus heate
d air has been investigated over a wide range of temperature, pressure
, and strain rate by numerical modeling with detailed chemistry and tr
ansport. Ignition temperatures calculated at constant strain rates are
seen to exhibit a Z-shaped pressure dependence similar to that observ
ed in explosion limits of homogeneous H-2/air mixtures. As with the co
rresponding explosion limits, the first and second ignition limits are
governed by the competition for hydrogen radicals between chain branc
hing (H + O-2 --> O + OH) and termination (H + O-2 + M --> HO2 + M) pa
thways, and the third ignition limit involves additional propagation (
2HO(2) --> H2O2 + O-2 --> 2OH + O-2) and branching (HO2 + H-2 --> H2O2
+ H --> 2OH + H) pathways that compete with chain termination. Igniti
on in this inhomogeneous, diffusive system is found to involve a spati
ally localized ignition ''kernel,'' identified as the region near the
point of maximum temperature where the rate of hydrogen radical chain
branching is maximized. Mass transport of radicals out of the ignition
kernel affects the ignition process by competing with chemical reacti
ons within the kernel, particularly in the first and third limits wher
e the dominant ignition chemistry is relatively slow. Ignition tempera
tures in these limits are found to be much more sensitive to aerodynam
ic straining than in the second limit. By controlling the width of the
ignition kernel and thus the characteristic residence time of key rad
icals within it, the strain rate is found to determine the dominant ch
emistry and the relevant ignition limit at any given pressure.