Crossed beam reaction of cyano radicals with hydrocarbon molecules. II. Chemical dynamics of 1-cyano-1-methylallene (CNCH3CCCH2; X (1)A(')) formationfrom reaction of CN(X (2)Sigma(+)) with dimethylacetylene CH3CCCH3 (X (1)A(1)('))
N. Balucani et al., Crossed beam reaction of cyano radicals with hydrocarbon molecules. II. Chemical dynamics of 1-cyano-1-methylallene (CNCH3CCCH2; X (1)A(')) formationfrom reaction of CN(X (2)Sigma(+)) with dimethylacetylene CH3CCCH3 (X (1)A(1)(')), J CHEM PHYS, 111(16), 1999, pp. 7472-7479
The reaction dynamics to form the 1-cyano-1-methylallene isomer CNCH3CCCH2
in its (1)A' ground state via the radical-closed shell reaction of the cyan
o radical CN(X (2)Sigma(+)) with dimethylacetylene CH3CCCH3 (X (1)A(1)') ar
e unraveled in a crossed molecular beam experiment at a collision energy of
20.8 kJ mol(-1) together with state-of-the-art electronic structure and Ri
ce-Ramsperger-Kassel-Marcus (RRKM) calculations. Forward convolution fittin
g of the laboratory angular distribution together with the time-of-flight s
pectra verify that the reaction is indirect and proceeds by addition of the
CN radical to the pi orbital to form a cis/trans CH3CNC=CCH3 radical inter
mediate. This decomposes via a rather lose exit transition state located on
ly 6-7 kJ mol(-1) above the products to CNCH3CCCH2 and atomic hydrogen. The
best fit of the center-of-mass angular distribution is forward-backward sy
mmetric and peaks at pi/2 documenting that the fragmenting intermediate hol
ds a lifetime longer than its rotational period. Further, the hydrogen atom
leaves almost perpendicular to the C5H5N plane resulting in sideways scatt
ering. This finding, together with low frequency bending and wagging modes,
strongly support our electronic structure calculations showing a H-C-C ang
le of about 106.5 degrees in the exit transition state. The experimentally
determined reaction exothermicity of 90 +/- 20 kJ mol(-1) is consistent wit
h the theoretical value, 80.4 kJ mol(-1). Unfavorable kinematics prevent us
from observing the CN versus CH3 exchange channel, even though our RRKM ca
lculations suggest that this pathway is more important. Since the title rea
ction is barrierless and exothermic, and the exit transition state is well
below the energy of the reactants, this process might be involved in the fo
rmation of unsaturated nitriles even in the coldest interstellar environmen
ts such as dark, molecular clouds and the saturnian satellite Titan. (C) 19
99 American Institute of Physics. [S0021-9606(99)01040-5].