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计算证据表明超共轭相互作用不是端基效应的原因。

Computational evidence that hyperconjugative interactions are not responsible for the anomeric effect.

机构信息

Department of Chemistry, Western Michigan University, Kalamazoo, Michigan 49008, USA.

出版信息

Nat Chem. 2010 Aug;2(8):666-71. doi: 10.1038/nchem.721. Epub 2010 Jul 4.

Abstract

The 'anomeric effect' is the thermodynamic preference for polar substituents to occupy the axial position in the chair conformation of various heterocycles. The most common explanation given for this effect at present is hyperconjugation from the lone pairs on the ring heteroatom to the antibonding orbital between the anomeric carbon and its linking substituent. Alternatively, the anomeric effect could be explained by intramolecular electrostatic interactions between local dipoles. Few models can provide convincing data for either theory at the quantum-mechanical level. Now, using the extended block-localized wavefunction method, which is the simplest form of valence bond theory, we have evaluated the degree of hyperconjugation in various compounds that display the anomeric effect and have interpreted their conformational preferences in terms of steric, hyperconjugation and dispersion effects. The results provide strong evidence that hyperconjugative interactions are not responsible for the anomeric effect and that it is better interpreted in terms of electrostatic interactions.

摘要

“端基效应”是指在各种杂环的椅式构象中,极性取代基倾向于占据轴向位置的热力学偏好。目前,对于这种效应最常见的解释是来自杂环原子上的孤对电子到端基碳原子与其连接取代基之间的反键轨道之间的超共轭。或者,端基效应可以通过分子内静电相互作用来解释。很少有模型可以在量子力学水平上为这两种理论提供令人信服的数据。现在,我们使用扩展的块局部波函数方法,这是价键理论的最简单形式,评估了在显示端基效应的各种化合物中超共轭的程度,并根据立体、超共轭和色散效应来解释它们的构象偏好。结果强烈表明超共轭相互作用不是端基效应的原因,而更好地用静电相互作用来解释。

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