Literature DB >> 26473337

Dynamics of the F(-) + CH3I → HF + CH2I(-) Proton Transfer Reaction.

Jiaxu Zhang1, Jing Xie2, William L Hase3.   

Abstract

Direct chemical dynamics simulations, at collision energies Erel of 0.32 and 1.53 eV, were performed to obtain an atomistic understanding of the F(-) + CH3I reaction dynamics. There is only the F(-) + CH3I → CH3F + I(-) bimolecular nucleophilic substitution SN2 product channel at 0.32 eV. Increasing Erel to 1.53 eV opens the endothermic F(-) + CH3I → HF + CH2I(-) proton transfer reaction, which is less competitive than the SN2 reaction. The simulations reveal proton transfer occurs by two direct atomic-level mechanisms, rebound and stripping, and indirect mechanisms, involving formation of the F(-)···HCH2I complex and the roundabout. For the indirect trajectories all of the CH2I(-) is formed with zero-point energy (ZPE), while for the direct trajectories 50% form CH2I(-) without ZPE. Without a ZPE constraint for CH2I(-), the reaction cross sections for the rebound, stripping, and indirect mechanisms are 0.2 ± 0.1, 1.2 ± 0.4, and 0.7 ± 0.2 Å(2), respectively. Discarding trajectories that do not form CH2I(-) with ZPE reduces the rebound and stripping cross sections to 0.1 ± 0.1 and 0.7 ± 0.5 Å(2). The HF product is formed rotationally and vibrationally unexcited. The average value of J is 2.6 and with histogram binning n = 0. CH2I(-) is formed rotationally excited. The partitioning between CH2I(-) vibration and HF + CH2I(-) relative translation energy depends on the treatment of CH2I(-) ZPE. Without a CH2I(-) ZPE constraint the energy partitioning is primarily to relative translation with little CH2I(-) vibration. With a ZPE constraint, energy partitioning to CH2I(-) rotation, CH2I(-) vibration, and relative translation are statistically the same. The overall F(-) + CH3I rate constant at Erel of both 0.32 and 1.53 eV is in good agreement with experiment and negligibly affected by the treatment of CH2I(-) ZPE, since the SN2 reaction is the major contributor to the total reaction rate constant. The potential energy surface and reaction dynamics for F(-) + CH3I proton transfer are compared with those reported previously (J. Phys. Chem. A 2013, 117, 7162-7178) for the isoelectronic OH(-) + CH3I reaction.

Year:  2015        PMID: 26473337     DOI: 10.1021/acs.jpca.5b08167

Source DB:  PubMed          Journal:  J Phys Chem A        ISSN: 1089-5639            Impact factor:   2.781


  3 in total

1.  High-level ab initio potential energy surface and dynamics of the F- + CH3I SN2 and proton-transfer reactions.

Authors:  Balázs Olasz; István Szabó; Gábor Czakó
Journal:  Chem Sci       Date:  2017-02-17       Impact factor: 9.825

2.  Stretching vibration is a spectator in nucleophilic substitution.

Authors:  Martin Stei; Eduardo Carrascosa; Alexander Dörfler; Jennifer Meyer; Balázs Olasz; Gábor Czakó; Anyang Li; Hua Guo; Roland Wester
Journal:  Sci Adv       Date:  2018-07-06       Impact factor: 14.136

3.  Imaging Proton Transfer and Dihalide Formation Pathways in Reactions of F(-) + CH3I.

Authors:  Eduardo Carrascosa; Tim Michaelsen; Martin Stei; Björn Bastian; Jennifer Meyer; Jochen Mikosch; Roland Wester
Journal:  J Phys Chem A       Date:  2016-02-05       Impact factor: 2.781

  3 in total

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