Formyl (HCO) radicals were generated in situ in the gas
phase via
the photolysis of glyoxal in N2 at 248 nm using the pulsed
laser photolysis–cavity ring-down spectrometry technique, and
the absorption cross-section of the radical was measured to be σHCO = (5.3 ± 0.9) × 10–19 cm2 molecule–1 at 298 K and 615.75 nm, which
was the probing wavelength. The kinetics of the reactions of HCO radicals
with ethyl formate (EF) and ethyl acetate (EA) were investigated experimentally
in the temperature range of 260–360 (±2) K at a pressure
of 60 Torr/N2. The absolute rate coefficient for the reaction
between HCO and EF was measured to be
(298 K) = (1.39 ± 0.30) × 10–14 cm3 molecule–1 s–1 at ambient temperature, whereas that for the reaction
of HCO with EA was measured tobe
(298 K) = (2.05 ± 0.43) × 10–14 cm3 molecule–1 s–1. The reaction of HCO with EA was faster than that
with EF, which might be due to the greater stability of the formed
radical intermediate due to hyperconjugative and inductive effects.
The dependency of the measured kinetics on experimental pressures
and laser fluences was examined within a certain range. To complement
the experiments, kinetics of the title reactions in the temperature
range of 200–400 K were deciphered theoretically via the canonical
variational transition-state theory with small-curvature tunneling
and interpolated single-point energy (CVT/SCT/ISPE) method using a
dual-level approach at the CCSD(T)/cc-pVTZ//MP2/6-311++G(d,p) level
of theory/basis set. A good degree of agreement was detected between
the rate coefficients measured experimentally and those calculated
theoretically both at room temperature and throughout the range of
temperatures studied. The kinetic branching ratios and thermochemistry
of the reactions were investigated to understand the thermodynamic
feasibility and kinetic lability of each pathway throughout the studied
temperatures. Atmospheric implications of these reactions of HCO radicals
are also discussed.