The rate of the reaction CH212 + H I 2 CH,I + I , has been followed spectrophotometrically from 201 .O to 31 1 .Z0. The rate constant for the reaction I + CH,I, CH,I + I, fits the equation, log (k,/M-'sec-') = 11.45 f 0.18 -(15.11 f 0.44)/0. This value, combined with the assumption that E2 = 0 & 1 k
A spectrokinetic study of CH2I and CH2IO2 radicals
β Scribed by Jens Sehested; Thomas Ellermann; Ole John Nielsen
- Book ID
- 102928032
- Publisher
- John Wiley and Sons
- Year
- 1994
- Tongue
- English
- Weight
- 775 KB
- Volume
- 26
- Category
- Article
- ISSN
- 0538-8066
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β¦ Synopsis
The UV absorption spectrum and kinetics of CHzI and CHzIOz radicals have been studied in the gasphase at 295 K using a pulse radiolysis W absorption spectroscopic technique. UV absorption spectra of CH2I and CHzIO2 radicals were quantified in the range 220-400 nm. The spectrum of CH2I has absorption maxima at 280 nm and 337.5 nm. The absorption cross-section for the CHzI radicals at 337.5 nm was (4.1 -C 0.9) x cm2 molecule-'. The UV spectrum of CHzIOz radicals is broad. The absorption cross-section at 370 nm was (2.1 5 0.5) X cm2 molecule-l. The rate constant for the self reaction of CH2I radicals, k = 4 X cm3 molecule-' s-' a t 1000 mbar total pressure of SFs, was derived by kinetic modelling of experimental absorbance transients. The observed self-reaction rate constant for CH2102 radicals was estimated also by modelling to k = 9 X 10-l' cm3 molecule-' s-'. As part of this work a rate constant of (2.0 % 0.3) X 10-lo cm3 molecule-' s-' was measured for the reaction of F atoms with CH3I. The branching ratios of this reaction for abstraction of an I atom and a H atom were determined to (64 -t 6)% and (36 2 6)%, respectively.
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Rate constants for the reactions of OH radicals and Cl atoms with CH,CH,NO>, CH,CH,CH,NO,, CH3CH2CH2CHzN02, and CH,CH2CH2CH,CH2N02 have been determined at 295+3 K and a total pressure of approximately 1 atm. The OH rate data were obtained using both the absolute rate technique of pulse radiolysis co
The structures ofcthylidcne and propylidene in their lowest singlet states :ue considered using INDO lnd MIND 112 calculations. Using a gadicnt optimization method, it is found that R!INDO/Z predicts no encrg minimu.n f-or singlet ethylidenc, while INDO predicts non-&ssic4 bridged structures for the