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镍(+)辅助丙醛分解中的浸没式屏障。

Submerged Barriers in the Ni(+) Assisted Decomposition of Propionaldehyde.

作者信息

Mansell A, Theis Z, Gutierrez M G, Faza O Nieto, Lopez C Silva, Bellert D J

机构信息

Department of Chemistry and Biochemistry, Baylor University , Waco, Texas 76798, United States.

Departamento de Quimica Organica, Universidad de Vigo , 36310, Vigo, Spain.

出版信息

J Phys Chem A. 2016 Apr 21;120(15):2275-84. doi: 10.1021/acs.jpca.5b08444. Epub 2016 Apr 7.

DOI:10.1021/acs.jpca.5b08444
PMID:27054589
Abstract

The reaction dynamics of the Ni(+) mediated decarbonylation of propionaldehyde was assessed using the single photon initiated decomposition rearrangement reaction (SPIDRR) technique. The exothermic production of Ni(+)CO was temporally monitored and the associated rate constants, k(E), were extracted as a function of activating photon energy. In addition, the reaction potential energy surface was calculated at the UCCSD(T)/def2-TZVP//PBEPBE/cc-pVDZ level of theory to provide an atomistic description of the reaction profile. The decarbonylation of propionaldehyde can be understood as proceeding through parallel competitive reaction pathways that are initiated by Ni(+) insertion into either the C-C or C-H bond of the propionaldehyde carbonyl carbon. Both paths lead to the elimination of neutral ethane and are governed by submerged barriers. The lower energy sequence is a consecutive C-C/C-H addition process with a submerged barrier of 14 350 ± 600 cm(-1). The higher energy sequence is a consecutive C-H/C-C addition process with a submerged barrier of 15 400 ± 600 cm(-1). Both barriers were determined using RRKM calculations fit to the experimentally determined k(E) values. The measured energy difference between the two barriers agrees with the DFT computed difference in rate limiting transition-state energies, 18 413 and 19 495 cm(-1).

摘要

采用单光子引发的分解重排反应(SPIDRR)技术评估了Ni(+)介导的丙醛脱羰反应动力学。对Ni(+)CO的放热生成进行了时间监测,并提取了相关的速率常数k(E)作为活化光子能量的函数。此外,在UCCSD(T)/def2-TZVP//PBEPBE/cc-pVDZ理论水平上计算了反应势能面,以提供反应历程的原子描述。丙醛的脱羰反应可以理解为通过平行竞争反应途径进行,这些途径由Ni(+)插入丙醛羰基碳的C-C键或C-H键引发。两条路径都导致中性乙烷的消除,并受潜势垒控制。能量较低的序列是一个连续的C-C/C-H加成过程,潜势垒为14 350 ± 600 cm(-1)。能量较高的序列是一个连续的C-H/C-C加成过程,潜势垒为15 400 ± 600 cm(-1)。这两个势垒均使用与实验测定的k(E)值拟合的RRKM计算确定。两个势垒之间测得的能量差与DFT计算的限速过渡态能量差18 413和19 495 cm(-1)一致。

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