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Investigation on the Thermal Dissociation of Vinyl Nitrite with a Saddle Point Involved

[Image: see text] Hybrid and double-hybrid density functionals are employed to explore the O–NO bond dissociation mechanism of vinyl nitrite (CH(2)=CHONO) into vinoxy (CH(2)=CHO) and nitric monoxide (NO). In contrast to previous investigations, which point out that the O–NO bond dissociation of viny...

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Detalles Bibliográficos
Autores principales: Guan, Yulei, Lou, Junpeng, Ma, Haixia, Song, Jirong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2019
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6777096/
https://www.ncbi.nlm.nih.gov/pubmed/31592473
http://dx.doi.org/10.1021/acsomega.9b02242
Descripción
Sumario:[Image: see text] Hybrid and double-hybrid density functionals are employed to explore the O–NO bond dissociation mechanism of vinyl nitrite (CH(2)=CHONO) into vinoxy (CH(2)=CHO) and nitric monoxide (NO). In contrast to previous investigations, which point out that the O–NO bond dissociation of vinyl nitrite is barrierless, our computational results clearly reveal that a kinetic barrier (first-order saddle point) in the O–NO bond dissociation is involved. Furthermore, a radical–radical adduct is recommended to be present on the dissociation path. The activation and reaction enthalpies at 298.15 K for the vinyl nitrite dissociation are calculated to be 91 and 75 kJ mol(–1) at the M062X/MG3S level, respectively, and the calculated reaction enthalpy compares very well with the experimental result of 76.58 kJ mol(–1). The M062X/MG3S reaction energetics, gradient, Hessian, and geometries are used to estimate vinyl nitrite dissociation rates based on the multistructural canonical variational transition-state theory including contributions from hindered rotations and multidimensional small-curvature tunneling at temperatures from 200 to 3000 K, and the rate constant results are fitted to the four-parameter Arrhenius expression of 4.2 × 10(9) (T/300)(4.3) exp[−87.5(T – 32.6)/(T(2) + 32.6(2))] s(–1).