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The ethylperoxy radical spectrum and rate constant for mutual interaction measured by flash photolysis and kinetic spectroscopy
Author(s) -
Adachi Hiroyuki,
Basco N.,
James D. G. L.
Publication year - 1979
Publication title -
international journal of chemical kinetics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.341
H-Index - 68
eISSN - 1097-4601
pISSN - 0538-8066
DOI - 10.1002/kin.550111107
Subject(s) - chemistry , radical , flash photolysis , absorbance , reaction rate constant , photodissociation , kinetic energy , photochemistry , analytical chemistry (journal) , absorption spectroscopy , yield (engineering) , molar absorptivity , kinetics , thermodynamics , organic chemistry , optics , physics , chromatography , quantum mechanics
Intrinsic spectral and kinetic parameters have been measured for the ethylperoxy radical, which was formed in the gas phase by the flash photolysis of azoethane in the presence of an adequate excess of oxygen. Absolute values of the extinction coefficient ϵ(λ) were derived from complementary measurements of the yield of nitrogen and the absorbance of an equivalent concentration of ethylperoxy radicals. The absorption spectrum is broad, structureless and comparatively weak; ϵ(236) = 1.02 × 10 3 liter mole −1 cm −1 at the maximum, and the oscillator strength is 3.4 × 10 −2 . This spectrum resembles the spectrum of the methylperoxy radical closely in form, but it is less intense; the ratio of the values of oscillator strength is 0.5. The bimolecular reactions of mutual interaction of ethylperoxy radicals are not exclusively terminating, and ethoxy and hydroperoxy radicals are formed in kinetically significant quantities. A computer program was designed to simulate the rise and fall of the concentration of each radical species, and to perform the related kinetic analysis. This program predicted that a second‐order plot of the decline of the absorbance of the ethylperoxy radical during the dark period would not show a significant departure from linearity, a conclusion which was confirmed by experiment. Accordingly, the gradient of each such plot yielded a value of k '/ϵ(λ), where k ' is the apparent value of the rate constant for the collective reactions of mutual interaction. This rate constant was evaluated from the product of corresponding values of k '/ϵ(λ) and ϵ(λ); individual values are independent of the wavelength of measurement, and the mean value is k ' = (6.6 ± 0.5) × 10 7 liter mole −1 sec −1 . Further kinetic analysis yielded the corresponding absolute value: k = (6.0 ± 0.6) × 10 7 liter mole −1 sec −1 . This value fits the pattern of a relationship between rate constant and structure shown by the methylperoxy, isopropylperoxy, and tert ‐butylperoxy radicals. Adequate sensitivity for the characterization of the spectrum of the ethylperoxy radical was achieved by the use of a pulsed xenon arc as the monitoring light source in conjunction with a dual beam detection system with twin cells and balanced photomultipliers, and the apparatus is described in detail.