Time-resolved IR spectral photography and transient diode laser absorp
tion measurements reveal a yield of HCl from the photolysis of Cl2 in
the presence of C2H5Cl and O2 which is 78% larger than expected from C
l + C2H5Cl. The HCl formation occurs in two steps: a rapid rise to [HC
l] = [Cl]0, followed by a secondary rise to [HCl] = 1.78[Cl]0 with a r
ate constant of k3 = (5.2 +/- 1.3) X 10(-12) cm3 S-1. In the presence
of NO, the rate of secondary HCl formation is greatly enhanced, but it
s yield (84%) is comparable to that in the absence of NO. The secondar
y HCl is explained as an elimination product from the CH3CHClO, which
can be generated by the reaction of CH3CHClO2 with itself or with NO.
The fact that the secondary HCl yield increases by 12% when using CD3C
H2Cl shows that the secondary HCl is formed mainly by three-center eli
mination from the 1-chloroethoxy radical. We also report UV absorption
cross sections for CH3CHClO2, which has a broad maximum of sigma(max)
= 0.029 angstrom2 from 215 to 248 nm, and CH2ClCH2O2, with sigma(max)
= 0.045 angstrom2 at 240 nm. The self-reaction rate constants are (5.
2+/-1.3) X 10(-12) cm3 s-l and (6.04-0.8) X 10(-12) cm3 s-1, respectiv
ely. Finally, the rate constant for the reaction Cl + C2H5Cl = C2H4Cl
+ HCl (1) is determined to be k1 = (7.3 +/- 0.9) X 10(-12) cm3 s-1.