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Spectroscopic identification and stability of the intermediate in the OH + HONO 2 reaction
The reaction of nitric acid with the hydroxyl radical influences the residence time of HONO 2 in the lower atmosphere. Prior studies [Brown SS, Burkholder JB, Talukdar RK, Ravishankara AR (2001) J Phys Chem A 105:1605–1614] have revealed unusual kinetic behavior for this reaction, including a negati...
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Published in: | Proceedings of the National Academy of Sciences - PNAS 2008-09, Vol.105 (35), p.12678-12683 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The reaction of nitric acid with the hydroxyl radical influences the residence time of HONO
2
in the lower atmosphere. Prior studies [Brown SS, Burkholder JB, Talukdar RK, Ravishankara AR (2001)
J Phys Chem A
105:1605–1614] have revealed unusual kinetic behavior for this reaction, including a negative temperature dependence, a complex pressure dependence, and an overall reaction rate strongly affected by isotopic substitution. This behavior suggested that the reaction occurs through an intermediate, theoretically predicted to be a hydrogen-bonded OH–HONO
2
complex in a six-membered ring-like configuration. In this study, the intermediate is generated directly by the association of photolytically generated OH radicals with HONO
2
and stabilized in a pulsed supersonic expansion. Infrared action spectroscopy is used to identify the intermediate by the OH radical stretch (ν
1
) and OH stretch of nitric acid (ν
2
) in the OH–HONO
2
complex. Two vibrational features are attributed to OH–HONO
2
: a rotationally structured ν
1
band at 3516.8 cm
−1
and an extensively broadened ν
2
feature at 3260 cm
−1
, both shifted from their respective monomers. These same transitions are identified for OD–DONO
2
. Assignments of the features are based on their vibrational frequencies, analysis of rotational band structure, and comparison with complementary high level
ab initio
calculations. In addition, the OH (
v
= 0) product state distributions resulting from ν
1
and ν
2
excitation are used to determine the binding energy of OH–HONO
2
,
D
0
≤ 5.3 kcal·mol
−1
, which is in good accord with
ab initio
predictions. |
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ISSN: | 0027-8424 1091-6490 |
DOI: | 10.1073/pnas.0800320105 |