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Recombination of Methyl Radicals. 1. New Data between 1175 and 1750 K in the Falloff Region
69
Citations
40
References
1996
Year
Radical EmissionEngineeringGeneticsRate CoefficientMolecular BiologyOptical AbsorptionAbsorption SpectroscopyChemistryMethyl RadicalsOptical DiagnosticsOptical PropertiesPhotophysical PropertyRadical (Chemistry)Nuclear AstrophysicsLaser PhotochemistryNatural SciencesSpectroscopyApplied PhysicsNew DataRecombination DynamicLight AbsorptionChemical KineticsFalloff Region
The rate coefficient for the recombination of methyl radicals, CH3 + CH3 → C2H6, was measured in incident shock-wave experiments on azomethane (0.12−1.3%) in argon. Methyl radicals were detected at 46 294 cm-1 (215.94 nm in air) by the tunable-laser flash-absorption technique. Postshock pressures between 114 and 230 kPa (1.13−2.27 atm) produced buffer gas concentrations between 5.4 × 1018 and 1.1 × 1019 cm-3. The cross section for optical absorption, the rate of dissociation of azomethane, and the rate coefficient of the recombinational reaction were determined simultaneously by least-squares analysis of methyl absorption profiles. The rate coefficient for the dissociation of azomethane from 850 to 1430 K is kdis(T) = 2.22 × 1039T-7.99 exp{−25920/T(K)} s-1. The temperature-dependent rate of recombination at 1.2 atm compares favorably with previous measurements. In terms of the phenomenological three-parameter equation of Kooji and the asymmetric Lorentzian broadening function of Gilbert et al., the recombination data from 296 to 1800 K may be described by k∞(T) = 1.53 × 10-7 T-1.203 exp{−295/T(K)} cm3s-1, k0(T) = 1.70 × 10-5T-7.248 exp{−2172/T(K)} cm6 s-1, and Fcent(T) = exp{−T(K)/506}.
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