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    Rate Constant and Branching Fraction for the NH<sub>2</sub> + NO<sub>2</sub> Reaction

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    The NH<sub>2</sub> + NO<sub>2</sub> reaction has been studied experimentally and theoretically. On the basis of laser photolysis/LIF experiments, the total rate constant was determined over the temperature range 295–625 K as <i>k</i><sub>1,exp</sub>(<i>T</i>) = 9.5 × 10<sup>–7</sup>(<i>T</i>/K)<sup>−2.05</sup> exp­(−404 K/<i>T</i>) cm<sup>3</sup> molecule<sup>–1</sup> s<sup>–1</sup>. This value is in the upper range of data reported for this temperature range. The reactions on the NH<sub>2</sub> + NO<sub>2</sub> potential energy surface were studied using high level ab initio transition state theory (TST) based master equation methods, yielding a rate constant of <i>k</i><sub>1,theory</sub>(<i>T</i>) = 7.5 × 10<sup>–12</sup>(<i>T</i>/K)<sup>−0.172</sup> exp­(687 K/<i>T</i>) cm<sup>3</sup> molecule<sup>–1</sup> s<sup>–1</sup>, in good agreement with the experimental value in the overlapping temperature range. The two entrance channel adducts H<sub>2</sub>NNO<sub>2</sub> and H<sub>2</sub>NONO lead to formation of N<sub>2</sub>O + H<sub>2</sub>O (R1a) and H<sub>2</sub>NO + NO (R1b), respectively. The pathways through H<sub>2</sub>NNO<sub>2</sub> and H<sub>2</sub>NONO are essentially unconnected, even though roaming may facilitate a small flux between the adducts. High- and low-pressure limit rate coefficients for the various product channels of NH<sub>2</sub> + NO<sub>2</sub> are determined from the ab initio TST-based master equation calculations for the temperature range 300–2000 K. The theoretical predictions are in good agreement with the measured overall rate constant but tend to overestimate the branching ratio defined as β = <i>k</i><sub>1a</sub>/(<i>k</i><sub>1a</sub> + <i>k</i><sub>1b</sub>) at lower temperatures. Modest adjustments of the attractive potentials for the reaction yield values of <i>k</i><sub>1a</sub> = 4.3 × 10<sup>–6</sup>(<i>T</i>/K)<sup>−2.191</sup> exp­(−229 K/<i>T</i>) cm<sup>3</sup> molecule<sup>–1</sup> s<sup>–1</sup> and <i>k</i><sub>1b</sub> = 1.5 × 10<sup>–12</sup>(<i>T</i>/K)<sup>0.032</sup> exp­(761 K/<i>T</i>) cm<sup>3</sup> molecule<sup>–1</sup> s<sup>–1</sup>, in good agreement with experiment, and we recommend these rate coefficients for use in modeling
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