Absorption spectroscopy has been applied to low-pressure, self-deflagrating
RDX flames in an attempt to refine the database for evaluation of detailed
-chemistry combustion models. Semi-empirically determined production rates
of reactants from the solid propellant surface together with a detailed gas
-phase elementary reaction set were used to develop a model that minimizes
the effect of uncertainties in the description of solid-phase processes. Th
e spatial profiles of two low-concentration, highly reactive, short-lived d
iatomic species, CN and NH, were obtained at pressures varying from 1 to 2
atm in air. Two major species, NO and OH were also profiled using this tech
nique. Resultant absorption spectra of the B(2)Sigma(+) - X(2)Sigma(+) tran
sitions for CN, A(3)II - X(3)Sigma(-) transitions for NH, and the A(2)Sigma
(+) - (XII)-I-2 transitions for NO and OH were least-squares fitted to obta
in best values for concentration and/or temperature. Peak CN mole fractions
of about 200 ppm are obtained from "snapshot" absorption spectra of RDX bu
rning in 1 atm air, mole fractions for NH are about a factor of 2 lower. As
the pressure is increased, the CN and NH species peak closer to the combus
ting surface and reside over a smaller spatial extent. Peak concentrations
drop for these higher pressures, but may be due, at least in part, to limit
ations of the spatial resolution of the pressurized absorption experiment c
hamber. Results from high-resolution absorption measurements instituted to
overcome these limitations reveal CN concentrations of 140 ppm with more co
nsistent peak positions, widths, and CN to NH peak ratios. Measurements of
the concentration of NO species show a peak concentration of 25 mole-percen
t occurring at a position of 0.12 mm above the surface of the propellant. I
n the final flame region, measured OH concentrations of 1.7 mole-percent ag
ree well with adiabatic calculations performed with the NASA-Lewis thermoch
emical equilibrium code. Calculated profiles of NO and OH are in good agree
ment with these measurements. Thr model peak positions and relative concent
rations of CN and NH are also in good agreement with experiment. During the
course of these spectroscopic measurements, burning rates for RDX over a p
ressure range of 1 to 2 atm have also been determined. These values range f
rom 0.23 mm/s at atmospheric pressure to 0.50 mm/s for 2 atm and are notice
ably lower than some of the other published measurements. Calculations stem
ming from the proposed model predict a burning rate of 0.29 mm/s and 0.54 m
m/s for the same pressure levels. (C) 1999 by The Combustion Institute.