Answers are grounded in this paper and cite their sources.
The infrared chemiluminescence of H 2 O and HOD molecules formed from the room-temperature reactions of OH and OD radicals with H 2 S, CH 3 SCH 3, and CH 3 SH was recorded by viewing a fast-flow reactor with a Fourier transform spectrometer. Nascent vibrational distributions of the H 2 O and HDO product molecules were obtained by computer simulation of the infrared spectra. According to our assignments for the v 3 = 0 populations, the vibrational distributions of HDO from the H 2 S and CH 3 SCH 3 reactions were inverted in the O−H stretching mode with a maximum in v 3 = 2 and v 3 = 1, respectively, and the fraction of the available energy released as vibrational energy is 〈 f v 〉 ≈ 0.6 with ∼25−30% of the vibrational energy in the bending coordinate. The reaction with CH 3 SH gives a HOD vibrational distribution that declines with increased v 3; 〈 f v 〉 is only ≈0.4, but 40% of the vibrational energy is in the bending mode. For each reaction, the vibrational distributions for H 2 O closely resemble those for HOD, after allowance is made for the collision-induced equilibration between the ν 1 and ν 3 modes of H 2 O and the ν 1 and 2ν 2 modes of HOD. The reduced vibrational energy disposal to H 2 O and HOD from CH 3 SH is taken as evidence for a mechanism that differs from the direct abstraction process for the H 2 S and CH 3 SCH 3 reactions. These results are analyzed using information theory, and they also are compared with the data from similar reactions of hydroxyl radicals and F atoms. Secondary reactions of the sulfur-containing primary radicals (SH, CH 3 S, and CH 3 SCH 2 ) with NO 2 and NO are discussed.
No takes yet. Share an insight, caveat, or question.
Butkovskaya et al. (1998) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: