Dr. Whitehouse et al., COMBUSTION OF STRATIFIED HYDROGEN-AIR MIXTURES IN THE 10.7 M(3) COMBUSTION TEST FACILITY CYLINDER, Nuclear Engineering and Design, 166(3), 1996, pp. 453-462
This paper presents preliminary results from hydrogen concentration gr
adient combustion experiments in a 10.7 m(3) cylinder. These gradients
, also referred to as stratified mixtures, were formed from dry mixtur
es of hydrogen and air at atmospheric temperature. Combustion pressure
s, burn fractions and flame speeds in concentration gradients were com
pared with combustion of well-mixed gases containing equivalent amount
s of hydrogen. The studied variables included the quantity of hydrogen
in the vessel, the steepness of the concentration gradient, the ignit
er location, and the initial concentration of hydrogen at the bottom o
f the vessel. Gradients of hydrogen and air with average concentration
s of hydrogen below the downward propagation limit produced significan
tly greater combustion pressures when ignited at the top of the vessel
than well-mixed gases with the same quantity of hydrogen. This was th
e result of considerably higher burn fractions in the gradients than i
n the well-mixed gas tests, Above the downward propagation limit, grad
ients of hydrogen ignited at the top of the vessel produced nearly the
same combustion pressures as under well-mixed conditions; both gradie
nts and well-mixed gases had high burn fractions. Much higher flame sp
eeds were observed in the gradients than the well-mixed gases. Gradien
ts and well-mixed gases containing up to 14%, hydrogen ignited at the
bottom of the vessel produced nearly the same combustion pressures. Ab
ove 14% hydrogen, gradients produced lower combustion pressures than w
ell-mixed gases having the same quantity of hydrogen. This can be attr
ibuted to lower burn fractions of fuel from the gradients compared wit
h well-mixed gases with similar quantities of hydrogen. When ignited a
t the bottom of the vessel, 90% of a gradient's gases remained unburne
d until several seconds after ignition. The remaining gases were then
consumed at a very fast rate.