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The Thermal Unimolecular Decomposition of Methyl Chloride behind Shock Waves
28
Citations
21
References
1980
Year
Materials ScienceShock WavesChemical EngineeringMolecular KineticsEngineeringDetonation PhenomenonPhysicsChemical ThermodynamicsNatural SciencesMethyl ChlorideThermal DecompositionPhysical ChemistryThermodynamicsChemistryHydrogenMolecular ChemistryChemical KineticsShock Compression
Abstract The thermal decomposition of methyl chloride diluted in Ar has been studied behind shock waves over the temperature range between 1680 and 2430 K and the total density range of 2.0×10−6–3.5×10−5 mol cm−3. The decomposition rate was monitored by means of the UV absorption of the CH3 radical produced. The initiation reaction was found to be the C–Cl bond fission; the process proceeded in the fall-off region under the present experimental conditions. From the fall-off data, low- and high-pressure rate constants (k0/[Ar] and k∞) were obtained by the application of a refined RRKM theory involving a weak collision effect. Thus, the Arrhenius expressions were given as: & k_0/[Ar]=10^15.56 exp(-247 kJ mol^-1/RT) cm^3 mol^-1 s^-1, & k_∞=10^13.86 exp(-383 kJ mol^-1/RT) s^-1. The collision efficiency factor, βc, was obtained as 0.02 at the mean temperature of the experiment by comparing the low-pressure rate constant with the strong collision-rate constant. The high-pressure rate constant was well explained by the maximum free-energy criterion presented by Quack and Troe.
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