Smith Madelyn, Li Zhen, Landry Luke, Merz Kenneth M, Li Pengfei
Department of Chemistry and Biochemistry, Loyola University Chicago, Chicago, Illinois 60660, United States.
Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, United States.
J Chem Theory Comput. 2023 Apr 11;19(7):2064-2074. doi: 10.1021/acs.jctc.2c01255. Epub 2023 Mar 23.
Atomic radii play important roles in scientific research. The covalent radii of atoms, ionic radii of ions, and van der Waals (VDW) radii of neutral atoms can all be derived from crystal structures. However, the VDW radii of ions are a challenge to determine because the atomic distances in crystal structures were determined by a combination of VDW interactions and electrostatic interactions, making it unclear how to define the VDW sphere of ions in such an environment. In the present study, we found that VDW radii, which were determined based on the 0.0015 au electron density contour through a wavefunction analysis on atoms, have excellent agreement with the VDW radii of noble-gas atoms determined experimentally. Based on this criterion, we calculated the VDW radii for various atomic ions across the periodic table, providing a systematic set of VDW radii of ions. Previously we have shown that the 12-6 Lennard-Jones nonbonded model could not simultaneously reproduce the hydration free energy (HFE) and ion-oxygen distance (IOD) for an atomic ion when its charge is +2 or higher. Because of this, we developed the 12-6-4 model to reproduce both properties at the same time by explicitly considering the ion-induced dipole interactions. However, recent studies showed it was possible to use the 12-6 model to simulate both properties simultaneously when an ion has the /2 parameter (., the VDW radius) close to the Shannon ionic radius. In the present study, we show that such a "success" is due to an unphysical overfitting, as the VDW radius of an ion should be significantly larger than its ionic radius. Through molecular dynamics simulations, we show that such overfitting causes significant issues when transferring the parameters from ion-water systems to ion-ligand and metalloprotein systems. In comparison, the 12-6-4 model shows significant improvement in comparison to the overfitted 12-6 model, showing excellent transferability across different systems. In summary, although both the 12-6-4 and 12-6 models could reproduce HFE and IOD for an ion, the 12-6-4 model accomplishes such a task based on the consideration of the physics involved, while the 12-6 model accomplishes this through overfitting, which brings significant transferability issues when simulating other systems. Hence, we strongly recommend the use of the 12-6-4 model (or even more sophisticated models) instead of overfitted 12-6 models when simulating complex systems such as metalloproteins.
原子半径在科学研究中发挥着重要作用。原子的共价半径、离子的离子半径以及中性原子的范德华(VDW)半径都可以从晶体结构中推导出来。然而,确定离子的VDW半径具有挑战性,因为晶体结构中的原子距离是由VDW相互作用和静电相互作用共同决定的,这使得在这种环境下不清楚如何定义离子的VDW球。在本研究中,我们发现通过对原子进行波函数分析,基于0.0015 au电子密度等值线确定的VDW半径与实验测定的稀有气体原子的VDW半径具有很好的一致性。基于这一标准,我们计算了整个周期表中各种原子离子的VDW半径,提供了一套系统的离子VDW半径。此前我们已经表明,当原子离子的电荷为 +2或更高时,12 - 6 Lennard - Jones非键模型不能同时再现其水化自由能(HFE)和离子 - 氧距离(IOD)。因此,我们开发了12 - 6 - 4模型,通过明确考虑离子诱导偶极相互作用来同时再现这两个性质。然而,最近的研究表明,当离子的 /2参数(即VDW半径)接近香农离子半径时,可以使用12 - 6模型同时模拟这两个性质。在本研究中,我们表明这种“成功”是由于非物理的过度拟合,因为离子的VDW半径应该明显大于其离子半径。通过分子动力学模拟,我们表明当将参数从离子 - 水系统转移到离子 - 配体和金属蛋白系统时,这种过度拟合会导致严重问题。相比之下,与过度拟合的12 - 6模型相比,12 - 6 - 4模型有显著改进,在不同系统中表现出出色的可转移性。总之,虽然12 - 6 - 4和12 - 6模型都可以再现离子的HFE和IOD,但12 - 6 - 4模型是基于对所涉及物理过程的考虑来完成这项任务的,而12 - 6模型是通过过度拟合来实现的,这在模拟其他系统时会带来严重的可转移性问题。因此,在模拟诸如金属蛋白等复杂系统时,我们强烈建议使用12 - 6 - 4模型(甚至更复杂的模型)而不是过度拟合的12 - 6模型。