Department of Chemistry, University of Massachusetts Amherst, Amherst, Massachusetts 01003, United States.
J Phys Chem B. 2024 Nov 28;128(47):11554-11564. doi: 10.1021/acs.jpcb.4c04777. Epub 2024 Nov 13.
Recent years have witnessed drastic improvements in general-purpose explicit solvent protein force fields, partially driven by the need to study intrinsically disordered proteins (IDPs), and yet the state-of-the-art force fields such as CHARMM36m (c36m) and a99SB-disp still provide different performances in simulating disordered protein states, where c36m has a bias toward overcompaction for large IDPs. Here, we examine the performance of c36m and a99SB-disp in describing the stabilities of a set of 46 amino acid backbone and side chain pairs in various configurations. The free energy results show that c36m systematically predicts stronger interactions compared to a99SB-disp by an average of 0.2 kcal/mol for nonpolar pairs, 0.6 kcal/mol for polar pairs, and 0.8 kcal/mol for salt bridges. The most severe overstabilization in c36m is observed for charged pairs involving the Arg and Glu side chains by up to 2.9 kcal/mol. Importantly, the systematic overstabilization of c36m is only marginally alleviated by c36mw, an patch to c36m that increases the dispersion interactions between TIP3P hydrogens and protein atoms. Guided by free energy decomposition, we evaluated if revising the charges alone could alleviate the severe overstabilization of salt bridges of c36m(w) vs a99SB-disp. The results suggested that the direct modification of protein-water interactions is also necessary. Toward this end, we proposed a tentative modification to c36m, referred to as c36mrb-disp, which combines modified Arg side chain charges, retuned backbone hydrogen bonding strength, and the a99SB-disp water model. The modified force field successfully reproduces the secondary structures of several intrinsically disordered peptides and proteins including (AAQAA), GB1p, and p53 transactivation domain, while maintaining the stability of a set of folded proteins. This work provides a set of useful systems for benchmarking and optimizing protein force fields and highlights the importance of balancing protein-protein and protein-water electrostatic interactions for accurately describing both folded and disordered proteins.
近年来,通用显式溶剂蛋白质力场取得了显著进展,部分原因是需要研究天然无序蛋白质 (IDP),但最先进的力场,如 CHARMM36m (c36m) 和 a99SB-disp,在模拟无序蛋白质状态时仍表现出不同的性能,其中 c36m 对大 IDP 有过度紧凑的偏差。在这里,我们检查了 c36m 和 a99SB-disp 在描述一组 46 个氨基酸骨架和侧链对各种构象的稳定性方面的性能。自由能结果表明,与 a99SB-disp 相比,c36m 系统地预测了更强的相互作用,非极性对平均为 0.2 kcal/mol,极性对为 0.6 kcal/mol,盐桥为 0.8 kcal/mol。在 c36m 中观察到最严重的过度稳定化是涉及 Arg 和 Glu 侧链的带电对,高达 2.9 kcal/mol。重要的是,c36m 的系统过度稳定化仅通过 c36mw 得到轻微缓解,c36mw 是对 c36m 的补丁,增加了 TIP3P 氢原子和蛋白质原子之间的色散相互作用。受自由能分解的指导,我们评估了仅修改电荷是否可以缓解 c36m(w) 与 a99SB-disp 之间盐桥的严重过度稳定化。结果表明,直接修改蛋白质-水相互作用也是必要的。为此,我们提出了对 c36m 的暂定修改,称为 c36mrb-disp,它结合了修改后的 Arg 侧链电荷、重新调整的骨架氢键强度和 a99SB-disp 水模型。改进的力场成功地再现了几个天然无序肽和蛋白质的二级结构,包括 (AAQAA)、GB1p 和 p53 转录激活结构域,同时保持了一组折叠蛋白的稳定性。这项工作为基准测试和优化蛋白质力场提供了一组有用的系统,并强调了平衡蛋白质-蛋白质和蛋白质-水静电相互作用对于准确描述折叠和无序蛋白质的重要性。