Influence of Iodine Merz–Singh–Kollman Radius on the Calculated Charges and Hydration Free Energies of Iodinated Molecules

Andreia Fortuna, Pedro M. S. Suzano, Miguel Machuqueiro, Paulo J. Costa
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Abstract

Empirical force field methods typically rely on point charges to describe the electrostatic interactions, which is problematic when anisotropy needs to be considered, as in the case of the electrostatic potential of covalently bound halogens that possess a positive site, termed σ-hole, surrounded by a large negative belt. To address this, an off-center point charge (extra point, EP) is usually placed at a given distance from the halogen to emulate the σ-hole and commonly used implementations are based on the restrained electrostatic potential (RESP) procedure to fit atomic charges, being one of the most used charge models. In this context, no specific Merz–Singh–Kollman (MK) radius for iodine is available in the literature, which is an essential parameter in the RESP fitting procedure. In this work, we explored the impact of the iodine MK radius on the obtained RESP charges for a set of 12 iodinated molecules. We verified that the relative root mean square (RRMS) values obtained with and without an EP kept decreasing with increasing radii for most compounds, thus impairing optimization using such a procedure. Nevertheless, the use of an iodine MK radius lower than 2 Å is not advisable since the RRMS kept decreasing considerably until this value was reached. Moreover, the performance of three iodine MK radii was studied with the estimation of the free energy of hydration (ΔGhyd) values using alchemical free energy calculations, which are particularly sensitive to the charges used. Despite the usage of different radii not leading to remarkable differences, our results indicate that using a value of 2.70 Å leads to lower mean absolute errors (MAE) and root mean squared error (RMSE) values when comparing the calculated with the experimental ΔGhyd values.

碘的默兹-辛格-科尔曼半径对碘化分子计算电荷和水合自由能的影响
经验力场方法通常依赖于点电荷来描述静电相互作用,当需要考虑各向异性时,这种方法就会出现问题,例如共价结合卤素的静电势,卤素具有一个被大负带包围的正位点,称为σ-孔。为了解决这个问题,通常会在距离卤素一定距离的地方放置一个偏离中心的点电荷(额外点,EP)来模拟σ-孔,常用的实现方法是基于约束静电势(RESP)程序来拟合原子电荷,这也是最常用的电荷模型之一。在这种情况下,文献中没有关于碘的特定 Merz-Singh-Kollman (MK) 半径,而该半径是 RESP 拟合程序中的一个重要参数。在这项工作中,我们探讨了碘的 MK 半径对一组 12 个含碘分子的 RESP 电荷的影响。我们证实,对于大多数化合物来说,使用和不使用 EP 所获得的相对均方根 (RRMS) 值随着半径的增大而不断减小,从而影响了使用这种程序进行优化。不过,使用半径小于 2 Å 的碘 MK 并不可取,因为在达到该值之前,RRMS 一直在大幅下降。此外,我们还利用炼金术自由能计算方法估算了水合自由能 (ΔGhyd),研究了三种碘 MK 半径的性能,该计算方法对所使用的电荷特别敏感。尽管使用不同的半径不会导致明显的差异,但我们的结果表明,在比较计算值和实验值 ΔGhyd 时,使用 2.70 Å 的值会导致较低的平均绝对误差 (MAE) 和均方根误差 (RMSE)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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