High level ab initio study of thermal 1,3-sigmatropic shift in CH2=CHCH2X with X = BH2, NH2, and CH3

High level ab initio study of thermal 1,3-sigmatropic shift in CH2=CHCH2X with X = BH2, NH2, and CH3
复制标题

DOI:
10.1021/jp025721u
复制
发表时间:
2002-06-13
影响因子:
2.9
通讯作者:
Lee, I
Lee, I
中科院分区:
化学3区
文献类型:
--
作者:
Choi, JY;Kim, CK;Lee, I

文献摘要

被引文献

相似文献

在RHF,MP2,B3 LYP,G3和CBS-APNO水平上,采用添加了扩散和极化函数的基组,研究了X-CH 2-CHCH 2(X = BH 2,NH 2和CH 3)体系的热1,3-σ迁移.在所有三种情况下,表面允许路径通过TS进行,其中CC π电子离域到迁移X中的2 p AO中。对于2 p空轨道的X = BH ~ 2,活化焓小于1.0 kcal mol ~(-1)(CBS-APNO),因此1,3-位移几乎是无势垒的.对于X = NH 2,有两条表面路径,其中一条(高能路径a)通过N上孤对电子的参与进行。较低能量路径的势垒高度(ΔH = 68.9 kcal mol-1)仅比C−N键的键离解能低1.0 kcal mol-1,因此双自由基路径可以与协同σ迁移竞争。对于X = CH 3,活化能垒(ΔH ε = 76.1 kcal mol-1)更高(约为1.2kcal mol-1)。1 kcal mol-1)比C1−X(CH 3)键的键离解能高,因此有利于双自由基反应路径。的antrafacial 1,3-移位被禁止在所有情况下,证明了二阶鞍点(有两个虚频率)和更高的势垒高度比相应的superfacial移位。
The thermal 1,3-sigmatropic migrations in X-CH2−CHCH2with X = BH2, NH2, and CH3have been investigated at the RHF, MP2, B3LYP, G3, and CBS-APNO levels using basis sets with added diffuse and polarization functions. In all three cases, the suprafacial allowed path proceeds through a TS in which the CC π electron is delocalized into the 2p AO in the migrating X. For X = BH2with a vacant 2p orbital, the activation enthalpy is less than 1.0 kcal mol-1(CBS-APNO) so that the 1,3-shift is almost barrierless. For X = NH2there are two suprafacial pathways, one of which (higher energy path a) proceeds by participation of the lone pair on N. The lower energy pathway has a barrier height (ΔH⧧= 68.9 kcal mol-1) of only 1.0 kcal mol-1below the bond dissociation energy of the C−N bond, so that a diradical pathway can compete with the concerted sigmatropic shift. For X = CH3, the activation barrier (ΔH⧧= 76.1 kcal mol-1) is higher (by ca. 1 kcal mol-1at the CBS-APNO level) than the bond dissociation energy of the C1−X(CH3) bond, so that the diradical reaction path is favored. The antrafacial 1,3-shifts are forbidden in all cases as evidenced by the second-order saddle-points (with two imaginary frequencies) and much higher barrier heights than those for the corresponding suprafacial shifts.