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Dissection of the Multichannel Reaction O((3)P) + C(2)H(2): Differential Cross-Sections and Product Energy Distributions

The O((3)P) + C(2)H(2) reaction plays an important role in hydrocarbon combustion. It has two primary competing channels: H + HCCO (ketenyl) and CO + CH(2) (triplet methylene). To further understand the microscopic dynamic mechanism of this reaction, we report here a detailed quasi-classical traject...

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Detalles Bibliográficos
Autores principales: Zhang, Shuwen, Chen, Qixin, Zuo, Junxiang, Hu, Xixi, Xie, Daiqian
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8838145/
https://www.ncbi.nlm.nih.gov/pubmed/35164017
http://dx.doi.org/10.3390/molecules27030754
Descripción
Sumario:The O((3)P) + C(2)H(2) reaction plays an important role in hydrocarbon combustion. It has two primary competing channels: H + HCCO (ketenyl) and CO + CH(2) (triplet methylene). To further understand the microscopic dynamic mechanism of this reaction, we report here a detailed quasi-classical trajectory study of the O((3)P) + C(2)H(2) reaction on the recently developed full-dimensional potential energy surface (PES). The entrance barrier TS1 is the rate-limiting barrier in the reaction. The translation of reactants can greatly promote reactivity, due to strong coupling with the reaction coordinate at TS1. The O((3)P) + C(2)H(2) reaction progress through a complex-forming mechanism, in which the intermediate HCCHO lives at least through the duration of a rotational period. The energy redistribution takes place during the creation of the long-lived high vibrationally (and rotationally) excited HCCHO in the reaction. The product energy partitioning of the two channels and CO vibrational distributions agree with experimental data, and the vibrational state distributions of all modes of products present a Boltzmann-like distribution.