Unimolecular decomposition kinetics of the stabilised Criegee intermediates CHOO and CDOO
Decomposition kinetics of stabilised CH 2 OO and CD 2 OO Criegee intermediates have been investigated as a function of temperature (450-650 K) and pressure (2-350 Torr) using flash photolysis coupled with time-resolved cavity-enhanced broadband UV absorption spectroscopy. Decomposition of CD 2 OO wa...
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Veröffentlicht in: | Physical chemistry chemical physics : PCCP 2018-10, Vol.2 (38), p.2494-24954 |
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Zusammenfassung: | Decomposition kinetics of stabilised CH
2
OO and CD
2
OO Criegee intermediates have been investigated as a function of temperature (450-650 K) and pressure (2-350 Torr) using flash photolysis coupled with time-resolved cavity-enhanced broadband UV absorption spectroscopy. Decomposition of CD
2
OO was observed to be faster than CH
2
OO under equivalent conditions. Production of OH radicals following CH
2
OO decomposition was also monitored using flash photolysis with laser-induced fluorescence (LIF), with results indicating direct production of OH in the
v
= 0 and
v
= 1 states in low yields. Master equation calculations performed using the Master Equation Solver for Multi-Energy well Reactions (MESMER) enabled fitting of the barriers for the decomposition of CH
2
OO and CD
2
OO to the experimental data. Parameterisations of the decomposition rate coefficients, calculated by MESMER, are provided for use in atmospheric models and implications of the results are discussed. For CH
2
OO, the MESMER fits require an increase in the calculated barrier height from 78.2 kJ mol
−1
to 81.8 kJ mol
−1
using a temperature-dependent exponential down model for collisional energy transfer with 〈Δ
E
〉
down
= 32.6(
T
/298 K)
1.7
cm
−1
in He. The low- and high-pressure limit rate coefficients are
k
1,0
= 3.2 × 10
−4
(
T
/298)
−5.81
exp(−12 770/
T
) cm
3
s
−1
and
k
1,∞
= 1.4 × 10
13
(
T
/298)
0.06
exp(−10 010/
T
) s
−1
, with median uncertainty of ∼12% over the range of experimental conditions used here. Extrapolation to atmospheric conditions yields
k
1
(298 K, 760 Torr) = 1.1
+1.5
−1.1
× 10
−3
s
−1
. For CD
2
OO, MESMER calculations result in 〈Δ
E
〉
down
= 39.6(
T
/298 K)
1.3
cm
−1
in He and a small decrease in the calculated barrier to decomposition from 81.0 kJ mol
−1
to 80.1 kJ mol
−1
. The fitted rate coefficients for CD
2
OO are
k
2,0
= 5.2 × 10
−5
(
T
/298)
−5.28
exp(−11 610/
T
) cm
3
s
−1
and
k
2,∞
= 1.2 × 10
13
(
T
/298)
0.06
exp(−9800/
T
) s
−1
, with overall error of ∼6% over the present range of temperature and pressure. The extrapolated
k
2
(298 K, 760 Torr) = 5.5
+9.2
−5.5
× 10
−3
s
−1
. The master equation calculations for CH
2
OO indicate decomposition yields of 63.7% for H
2
+ CO
2
, 36.0% for H
2
O + CO and 0.3% for OH + HCO with no significant dependence on temperature between 400 and 1200 K or pressure between 1 and 3000 Torr.
Decomposition kinetics of stabilised CH
2
OO and CD
2
OO Criegee intermediates have been investigated as a function of temperature (4 |
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ISSN: | 1463-9076 1463-9084 |
DOI: | 10.1039/c8cp05332d |