Volume 93, Issue 1 pp. 80-87
Article
Full Access

The reaction of CH2(X̄3B1) with C6H6

T. Böhland

T. Böhland

Max-Planck-Institut für Strömungsforschung, Bunsenstraße 10, D-3400 Göttingen, West-Germany

Search for more papers by this author
K. Héberger

K. Héberger

Max-Planck-Institut für Strömungsforschung, Bunsenstraße 10, D-3400 Göttingen, West-Germany

Central Research Institute for Chemistry of the Hungarian Academy of Sciences, Pusztaszeri ut 59–67, H-1025 Budapest, Hungary.

Search for more papers by this author
F. Temps

F. Temps

Max-Planck-Institut für Strömungsforschung, Bunsenstraße 10, D-3400 Göttingen, West-Germany

Search for more papers by this author
H. Gg. Wagner

H. Gg. Wagner

Max-Planck-Institut für Strömungsforschung, Bunsenstraße 10, D-3400 Göttingen, West-Germany

Search for more papers by this author
First published: Januar 1989
Citations: 10

Abstract

The kinetics of the reaction CH2(X̄3B1) + C6H6 → products (1) has been studied in a discharge flow reactor using Laser Magnetic Resonance (LMR) detection for CH2. The experiments yielded the overall rate constant kexp1 = (4.7 ± 2.4) · 10t3 exp(−(37.5 ± 2.4) kJ mol−1/RT) in the temperature range 448 K ≦T ≦ 683 K. The product formation was investigated for reaction (1) as well as the corresponding reaction CH21A1) + C6H6 → products (2) in a stationary photolysis reactor employing gas chromatographic analysis by photolyzing mixtures of CH2CO and C6H6 at λ1 = 366 nm and λ2 = 313 nm. The relative yields of the products cycloheptatriene (CHT) and toluene (T) were found to depend on the wavelength, [T]/([CHT] + [T]) = (0.13 ± 0.02) and (0.23 ± 0.02) at λ1, and λ2, respectively. The implications of these results and the mechanisms are discussed.

The full text of this article hosted at iucr.org is unavailable due to technical difficulties.