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The UV absorption spectrum of the CCl 3 radical and the kinetics of its mutual combination reaction from 253 to 623 K
Author(s) -
Danis F.,
Caralp F.,
Veyret B.,
Loirat H.,
Lesclaux R.
Publication year - 1989
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.550210810
Subject(s) - chemistry , flash photolysis , reaction rate constant , kinetics , radical , analytical chemistry (journal) , absorption spectroscopy , absorption (acoustics) , photodissociation , torr , atmospheric temperature range , absorption cross section , photochemistry , thermodynamics , cross section (physics) , organic chemistry , physics , quantum mechanics , acoustics
The UV absorption spectrum and the kinetics of the self combination reaction of the CCl 3 radical were studied by flash photolysis in the temperature range 253–623 K. Experiments were performed at the atmospheric pressure, except for a few runs at the highest temperatures, which were performed between 30 and 760 torr. CCl 3 radicals were generated by flash photolysis of molecular chlorine in the presence of chloroform. The UV spectrum exhibits a strong unstructured band between 195 and 260 nm with a maximum at 211 ± 2 nm. The absorption cross section, measured relative to σ(HO 2 ), is σ(CCl 3 ) = (1.45 ± 0.35) × 10 −17 cm 2 molecule −1 at the maximum. This value takes into account the uncertainty in σ(HO 2 ) which was taken equal to (4.9 ± 0.7) × 10 −18 cm 2 molecule −1 . The absolute rate constant for the CCl 3 mutual combination was determined by computer simulation of the transient decays. The rate constant, which exhibits a slight negative temperature coefficient, can be expressed as:\documentclass{article}\pagestyle{empty}\begin{document}$$ k_6 = (3.3 \pm 0.8) \times 10^{- 12} (T/298)^{- 1.0 \pm 0.2} {\rm cm}^{\rm 3} {\rm molecule}^{- 1} {\rm s}^{- 1} {\rm at 760 torr}{\rm.} $$\end{document}The study of the pressure dependence showed that only a slight fall‐off behavior could be observed at the highest temperature (623 K). This result was corroborated by RRKM calculations which showed that the rate constant is at the high pressure limit under most experimental conditions below 600 K.