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首页> 外文期刊>Journal of Computational Chemistry: Organic, Inorganic, Physical, Biological >A MOLECULAR MECHANICAL MODEL THAT REPRODUCES THE RELATIVE ENERGIES FOR CHAIR AND TWIST-BOAT CONFORMATIONS OF 1,3-DIOXANES
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A MOLECULAR MECHANICAL MODEL THAT REPRODUCES THE RELATIVE ENERGIES FOR CHAIR AND TWIST-BOAT CONFORMATIONS OF 1,3-DIOXANES

机译:分子机械模型,可再现1,3-二恶烷的椅子和扭曲骨架构型的相对能量

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We present molecular mechanics calculations on the conformational energies of several `2,2-dimethyl-trans-4,6-disubstituted-1,3-dioxanes. Previous studies by Rychnovsky et al. have suggested that the relative conformational energies of chair and twist-boat forms of these 1,3-dioxanes were poorly represented by the molecular mechanical models MM2* and MM3* (MacroModel implementations of MM2 and MM3) both when compared to experiment and to high-level quantum mechanical calculations. We have studied these molecules with a molecular mechanical force field which features electrostatic-potential-based atomic charges. This model does an excellent job of reproducing the relative conformational energies of the highest level of theory (MP2/6-31G*) applied to the problem. Furthermore, when empirically corrected using the MP2/6-31G* relative conformational energies of the unsubstituted compound 2,2,4-trimethyl-1,3-dioxane, the absolute energy differences calculated with this new model between the chair and twist-boat conformers for five substituted compounds are within an average of 0.30 kcal/mol of the MP2/6-31G* values. The correlation with experiment is also very good. One can, however, modify the initial molecular mechanical model with a single V-1(-O-C-O-C-) torsional potential and do an excellent job in reproducing the absolute conformational energies of the dioxanes as well, with an average error in conformational energies of 0.45 kcal/mol. This same torsional potential was independently developed by comparing ab initio and molecular mechanical energies of the molecule 1,1-dimethoxymethane. Thus, we have succeeded in developing a general molecular mechanical model for 1,3-dioxoalkanes. In addition, we have compared the standard MM2 and MM3 models with MM2* and MM3* (ref. 2) and have found some significant differences in relative conformational energies between MM2 and MM2*. MM2 has an improved correlation with the best ab initio data compared to MM2* but is still significantly worse than that found with lower-level ab initio or AM1 semiempirical quantum mechanics or the new molecular mechanical model presented here. MM3 leads to conformational energies very similar to MM3*. Energy component analysis suggests that the single most important element in reproducing the conformational equilibrium is the electrostatic energy. This fact rationalizes the success of AMBER models, whose fundamental tenet is the accurate representation of quantum mechanically calculated molecular electrostatic effects. (C) 1995 by John Wiley and Sons, Inc. [References: 19]
机译:我们目前对几种`2,2-二甲基-反式-4,6-二取代-1,3-二恶烷的构象能进行分子力学计算。 Rychnovsky等人先前的研究。已经表明,与实验相比和较高时,分子力学模型MM2 *和MM3 *(MM2和MM3的宏模型实现)无法很好地表示这些1,3-二恶烷的椅形和扭转舟形相对构象能级量子力学计算。我们已经研究了具有分子机械力场的这些分子,该场具有基于静电势的原子电荷。该模型在再现应用于该问题的最高理论水平(MP2 / 6-31G *)的相对构象能量方面做得非常出色。此外,当使用未经取代的化合物2,2,4-三甲基-1,3-二恶烷的MP2 / 6-31G *相对构象能量进行经验校正时,使用此新模型计算出的椅子和扭艇之间的绝对能量差五个取代化合物的构象异构体平均MP2 / 6-31G *值在0.30 kcal / mol之内。与实验的相关性也很好。但是,可以用单个V-1(-OCOC-)扭转势来修改初始分子力学模型,并且在重现二恶烷的绝对构象能方面也能做得很好,构象能的平均误差为0.45大卡/摩尔通过比较分子1,1-二甲氧基甲烷的从头算和分子机械能,可以独立地开发出相同的扭转势。因此,我们已经成功地开发了1,3-二氧代链烷烃的一般分子力学模型。此外,我们将标准的MM2和MM3模型与MM2 *和MM3 *(参考文献2)进行了比较,发现MM2和MM2 *之间的相对构象能存在一些显着差异。与MM2 *相比,MM2与最佳的从头算数据具有更好的相关性,但仍然比在较低水平的从头算术或AM1半经验量子力学或此处介绍的新分子力学模型中发现的更好。 MM3产生的构象能量与MM3 *非常相似。能量成分分析表明,重现构象平衡中最重要的元素是静电能。这一事实使AMBER模型的成功合理化,其基本宗旨是精确地表示量子力学计算的分子静电效应。 (C)1995年,John Wiley and Sons,Inc. [参考:19]

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