Campanelli Anna Rita, Domenicano Aldo, Ramondo Fabio, Hargittai István
Department of Chemistry, University of Rome "La Sapienza", I-00185 Rome, Italy.
J Phys Chem A. 2008 Oct 30;112(43):10998-1008. doi: 10.1021/jp803425h. Epub 2008 Oct 4.
The molecular structures of cyanobenzene, p-dicyanobenzene, and 1,2,4,5-tetracyanobenzene have been accurately determined by gas-phase electron diffraction and ab initio/DFT MO calculations. The equilibrium structures of these molecules are planar, but their average geometries in the gaseous phase are nonplanar because of large-amplitude vibrational motions of the substituents out of the plane of the benzene ring. The use of nonplanar models in electron diffraction analysis is necessary to yield ring angles consistent with the results of MO calculations. The angular deformation of the benzene ring in the three molecules is found to be much smaller than obtained from previous electron diffraction studies, as well as from microwave spectroscopy studies of cyanobenzene. While the deformation of the ring CC bonds and CCC angles in p-dicyanobenzene is well interpreted as arising from the superposition of independent effects from each substituent, considerable deviation from additivity occurs in 1,2,4,5-tetracyanobenzene. The changes in the ring geometry and C ipso-C cyano bond lengths in this molecule indicate an enhanced ability of the cyano group to withdraw pi-electrons from the benzene ring, compared with cyanobenzene and p-dicyanobenzene. In particular, gas-phase electron diffraction and MP2 or B3LYP calculations show a small but consistent increase in the mean length of the ring CC bonds for each cyano group and a further increase in 1,2,4,5-tetracyanobenzene. Comparison with accurate results from X-ray and neutron crystallography indicates that in p-dicyanobenzene the internal ring angle at the place of substitution opens slightly as the molecule is frozen in the crystal. The small geometrical change, about 0.6 degrees , is shown to be real and to originate from intermolecular C identical withN...HC interactions in the solid state.
通过气相电子衍射和从头算/密度泛函理论分子轨道计算,已精确测定了氰基苯、对二氰基苯和1,2,4,5-四氰基苯的分子结构。这些分子的平衡结构是平面的,但由于取代基在苯环平面外的大幅度振动,它们在气相中的平均几何形状是非平面的。在电子衍射分析中使用非平面模型对于得到与分子轨道计算结果一致的环角是必要的。发现这三种分子中苯环的角变形比先前电子衍射研究以及氰基苯的微波光谱研究所得结果小得多。虽然对二氰基苯中环碳碳键和碳碳碳角的变形可以很好地解释为每个取代基独立作用的叠加,但在1,2,4,5-四氰基苯中出现了与加和性的显著偏差。与氰基苯和对二氰基苯相比,该分子中环几何形状和C本位-C氰基键长的变化表明氰基从苯环中提取π电子的能力增强。特别是,气相电子衍射和MP2或B3LYP计算表明,每个氰基的环碳碳键平均长度有小但一致的增加,并且在1,2,4,5-四氰基苯中进一步增加。与X射线和中子晶体学的精确结果比较表明,在对二氰基苯中,当分子在晶体中冻结时,取代位置处的内环角略有张开。约0.6度的小几何变化被证明是真实的,并且源于固态下分子间C≡N...HC相互作用。