Tamar SteinLene Krogh ChristensenJ. PlatzJens SehestedOle John NielsenTimothy J. Wallington
Pulse radiolysis transient UV absorption spectroscopy was used to study the ultraviolet absorption spectra (230−330 nm) and kinetics of CF3C(O)OCH(·)CF3 and CF3C(O)OCH(OO·)CF3 radicals at 296 K. At 280 nm σ(CF3C(O)OCH(·)CF3) = (1.08 ± 0.13) × 10-18 cm2 molecule-1, at 240 nm σ(CF3C(O)OCH(OO·)CF3) = (2.06 ± 0.24) × 10-18 cm2 molecule-1. Rate constants for the reaction of F atoms with CF3C(O)OCH2CF3, the self-reactions of CF3C(O)OCH(·)CF3 and CF3C(O)OCH(OO·)CF3 radicals, and the reactions of CF3C(O)OCH(OO·)CF3 radicals with NO and NO2 were (1.8 ± 0.2) × 10-12, (1.5 ± 0.2) × 10-11, (7.6 ± 0.9) × 10-12, (1.5 ± 0.2) × 10-11, and (8.5 ± 0.9) × 10-12 cm3 molecule-1 s-1, respectively. The atmospheric fate of CF3C(O)OCH(O·)CF3 radicals was investigated in a FTIR smog chamber. Three loss processes for the CF3C(O)OCH(O·)CF3 radicals were identified at 296 K and 700 Torr total pressure, reaction with O2 to form CF3C(O)OC(O)CF3, α-rearrangement to form CF3C(O)· radicals and CF3C(O)OH, and decomposition via a mechanism which is unclear. In 760 Torr of air at 296 K, 65% of the CF3C(O)OCH(O·)CF3 radicals react with oxygen, 18% undergo α-rearrangement, while the fate of the remaining 17% is unclear.
Timothy J. WallingtonA. GuschinTamar SteinJ. PlatzJens SehestedLene Krogh ChristensenOle John Nielsen
Freja F. ØsterstrømTimothy J. WallingtonMads P. Sulbæk AndersenOle John Nielsen
Freja F. ØsterstrømTimothy J. WallingtonMads P. Sulbæk AndersenOle John Nielsen
Rodion KopitzkyHelge WillnerAngelika HermannHeinz Oberhammer
Kanika GuleriaRanga Subramanian