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Accuracy of continuum electrostatic calculations based on three common dielectric boundary definitions

机译:基于三种常见介电边界定义的连续静电计算的准确性

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摘要

We investigate the influence of three common definitions of the solute/solvent dielectric boundary (DB) on the accuracy of the electrostatic solvation energy ΔGel computed within the Poisson Boltzmann and the generalized Born models of implicit solvation. The test structures include small molecules, peptides and small proteins; explicit solvent ΔGel are used as accuracy reference. For common atomic radii sets BONDI, PARSE (and ZAP9 for small molecules) the use of van der Waals (vdW) DB results, on average, in considerably larger errors in ΔGel than the molecular surface (MS) DB. The optimal probe radius ρw for which the MS DB yields the most accurate ΔGel varies considerably between structure types. The solvent accessible surface (SAS) DB becomes optimal at ρw ~ 0.2 Å (exact value is sensitive to the structure and atomic radii), at which point the average accuracy of ΔGel is comparable to that of the MS-based boundary. The geometric equivalence of SAS to vdW surface based on the same atomic radii uniformly increased by ρw gives the corresponding optimal vdW DB. For small molecules, the optimal vdW DB based on BONDI + 0.2 Å radii can yield ΔGel estimates at least as accurate as those based on the optimal MS DB. Also, in small molecules, pairwise charge-charge interactions computed with the optimal vdW DB are virtually equal to those computed with the MS DB, suggesting that in this case the two boundaries are practically equivalent by the electrostatic energy criteria. In structures other than small molecules, the optimal vdW and MS dielectric boundaries are not equivalent: the respective pairwise electrostatic interactions in the presence of solvent can differ by up to 5 kcal/mol for individual atomic pairs in small proteins, even when the total ΔGel are equal. For small proteins, the average decrease in pairwise electrostatic interactions resulting from the switch from optimal MS to optimal vdW DB definition can be mimicked within the MS DB definition by doubling of the solute dielectric constant. However, the use of the higher interior dielectric does not eliminate the large individual deviations between pairwise interactions computed within the two DB definitions. It is argued that while the MS based definition of the dielectric boundary is more physically correct in some types of practical calculations, the choice is not so clear in some other common scenarios.
机译:我们研究了三种常见的溶质/溶剂介电边界(DB)定义对在Poisson Boltzmann和广义Born隐式溶剂化模型中计算的静电溶剂化能量ΔGel的准确性的影响。测试结构包括小分子,肽和小蛋白质。显式溶剂ΔGel用作准确度参考。对于常见的原子半径集BONDI,PARSE(对于小分子,则为ZAP9),使用范德华(vdW)DB平均而言,ΔGel的误差要比分子表面(MS)DB大得多。 MS DB产生最准确的ΔGel的最佳探针半径ρw在结构类型之间有很大差异。溶剂可及表面(SAS)DB在ρw〜0.2Å(精确值对结构和原子半径敏感)时变得最佳,此时ΔGel的平均准确度可与基于MS的边界相比较。基于相同的原子半径,将SAS与vdW表面的几何当量均匀地增加ρw,可以得到相应的最佳vdW DB。对于小分子,基于BONDI + 0.2半径的最佳vdW DB可以产生的ΔGel估计值至少与基于最佳MS DB的估计值一样准确。同样,在小分子中,用最佳vdW DB计算出的成对电荷-电荷相互作用实际上等于用MS DB计算出的电荷-电荷相互作用,这表明在这种情况下,两个边界实际上符合静电能标准。在除小分子以外的结构中,最佳vdW和MS介电边界不相等:对于小蛋白质中的单个原子对,在溶剂存在下各自的成对静电相互作用可能相差5 kcal / mol,即使总ΔGel相等。对于小蛋白质,可以通过将溶质介电常数加倍,来模拟从最佳MS切换到最佳vdW DB定义所导致的成对静电相互作用的平均下降。但是,使用较高的内部电介质并不能消除在两个DB定义中计算的成对相互作用之间的较大个体偏差。有人认为,尽管在某些类型的实际计算中,基于MS的介电边界定义在物理上更为正确,但在其他一些常见情况下,选择却不是那么明确。

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  • 年(卷),期 -1(13),3
  • 年度 -1
  • 页码 1440006
  • 总页数 31
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