Wrass John P, Sadowsky Daniel, Bloomgren Kaitlin M, Cramer Christopher J, Phillips James A
Department of Chemistry, University of Wisconsin Eau-Claire, Eau Claire, WI 54702, USA.
Phys Chem Chem Phys. 2014 Aug 21;16(31):16480-91. doi: 10.1039/c4cp01495b.
We have characterized the structural and energetic properties of CH3CN-BCl3via computations and matrix-IR spectroscopy. We find two equilibrium structures of the complex via computations. At the MP2/aug-cc-pVTZ level, the global minimum energy structure has a B-N distance of 1.601 Å, and a binding energy of 12.0 kcal mol(-1). The secondary structure lies 7.1 kcal mol(-1) higher in energy with a B-N distance of 2.687 Å and a binding energy of 4.9 kcal mol(-1). Computational scans of the B-N potential curve using both DFT and post-HF methods indicate that a significant barrier exists between these structures, and that it lies 1 to 2 kcal mol(-1) above the secondary minimum at a B-N distance of about 2.2 Å. We also observed several key, structurally-sensitive IR bands for six isotopic forms of the complex in neon matrices, including: the B-Cl asymmetric stretching band (ν) at 792 cm(-1) and the C-N stretching band (νCN) at 2380 cm(-1) (for the primary isotopomer, CH3C(14)N-(11)BCl3). These frequencies are consistent with computational predictions for the minimum-energy form of the complex. Energy decomposition analyses were conducted for CH3CN-BCl3 and also two related complexes, CH3CN-BF3 and CH3CN-BH3. These provide insight into the trend in Lewis acidity of the BX3 acceptors toward nitriles. Furthermore, these analyses indicate that the barrier along the B-N potential of CH3CN-BCl3 results from Pauli repulsion between the π electrons on the nitrile moiety and the chlorine atoms in BCl3, which is significant at relatively long distances where attractive bonding interactions fail to overcome it.
我们通过计算和矩阵红外光谱对CH3CN - BCl3的结构和能量性质进行了表征。通过计算我们发现该配合物有两种平衡结构。在MP2/aug - cc - pVTZ水平下,全局最低能量结构的B - N距离为1.601 Å,结合能为12.0 kcal mol(-1)。二级结构的能量比全局最低能量结构高7.1 kcal mol(-1),B - N距离为2.687 Å,结合能为4.9 kcal mol(-1)。使用密度泛函理论(DFT)和后哈特里 - 福克(post - HF)方法对B - N势能曲线进行的计算扫描表明,这些结构之间存在一个显著的势垒,并且在B - N距离约为2.2 Å时,该势垒比二级最小值高1至2 kcal mol(-1)。我们还在氖基质中观察到了该配合物六种同位素形式的几个关键的、对结构敏感的红外波段,包括:792 cm(-1)处的B - Cl不对称伸缩带(ν)和2380 cm(-1)处的C - N伸缩带(νCN)(对于主要同位素异构体CH3C(14)N - (11)BCl3)。这些频率与该配合物最低能量形式的计算预测结果一致。对CH3CN - BCl3以及另外两个相关配合物CH3CN - BF3和CH3CN - BH3进行了能量分解分析。这些分析为BX3受体对腈的路易斯酸性趋势提供了见解。此外,这些分析表明,CH3CN - BCl3沿B - N势的势垒是由腈基部分的π电子与BCl3中的氯原子之间的泡利排斥引起的,在相对较长的距离上这种排斥作用很显著,此时吸引性的键合相互作用无法克服它。