Skaggs School of Pharmacy and Pharmaceutical Sciences, University of California San Diego, 9500 Gilman Drive, La Jolla, California 92093-0736, USA.
J Chem Phys. 2012 Jul 28;137(4):044101. doi: 10.1063/1.4733951.
The displacement of perturbed water upon binding is believed to play a critical role in the thermodynamics of biomolecular recognition, but it is nontrivial to unambiguously define and answer questions about this process. We address this issue by introducing grid inhomogeneous solvation theory (GIST), which discretizes the equations of inhomogeneous solvation theory (IST) onto a three-dimensional grid situated in the region of interest around a solute molecule or complex. Snapshots from explicit solvent simulations are used to estimate localized solvation entropies, energies, and free energies associated with the grid boxes, or voxels, and properly summing these thermodynamic quantities over voxels yields information about hydration thermodynamics. GIST thus provides a smoothly varying representation of water properties as a function of position, rather than focusing on hydration sites where solvent is present at high density. It therefore accounts for full or partial displacement of water from sites that are highly occupied by water, as well as for partly occupied and water-depleted regions around the solute. GIST can also provide a well-defined estimate of the solvation free energy and therefore enables a rigorous end-states analysis of binding. For example, one may not only use a first GIST calculation to project the thermodynamic consequences of displacing water from the surface of a receptor by a ligand, but also account, in a second GIST calculation, for the thermodynamics of subsequent solvent reorganization around the bound complex. In the present study, a first GIST analysis of the molecular host cucurbit[7]uril is found to yield a rich picture of hydration structure and thermodynamics in and around this miniature receptor. One of the most striking results is the observation of a toroidal region of high water density at the center of the host's nonpolar cavity. Despite its high density, the water in this toroidal region is disfavored energetically and entropically, and hence may contribute to the known ability of this small receptor to bind guest molecules with unusually high affinities. Interestingly, the toroidal region of high water density persists even when all partial charges of the receptor are set to zero. Thus, localized regions of high solvent density can be generated in a binding site without strong, attractive solute-solvent interactions.
据信,扰动水在结合时的位移在生物分子识别的热力学中起着关键作用,但要明确定义并回答有关该过程的问题并非易事。我们通过引入网格不均匀溶剂化理论(GIST)来解决这个问题,该理论将不均匀溶剂化理论(IST)的方程离散到位于溶质分子或复合物周围感兴趣区域的三维网格上。来自显式溶剂模拟的快照用于估计与网格盒或体素相关的局部溶剂化熵、能量和自由能,并通过体素正确地对这些热力学量求和,可获得有关水合热力学的信息。因此,GIST 提供了一种平滑变化的水性质表示,而不是关注溶剂高密度存在的水合位置。因此,它既考虑了从高度被水占据的位置完全或部分置换水的情况,也考虑了溶质周围部分占据和缺水的区域。GIST 还可以提供溶剂化自由能的明确定义估计,从而能够对结合进行严格的末端状态分析。例如,人们不仅可以使用第一次 GIST 计算来预测配体从受体表面置换水的热力学后果,还可以在第二次 GIST 计算中考虑围绕结合复合物的随后溶剂重组的热力学。在本研究中,对分子主体葫芦[7]脲的第一次 GIST 分析得出了该微型受体内部和周围水合结构和热力学的丰富图像。最引人注目的结果之一是观察到主体非极性腔中心的高水密度环形区域。尽管水密度很高,但这种环形区域在能量和熵上都不受欢迎,因此可能有助于该小型受体以异常高的亲和力结合客体分子的已知能力。有趣的是,即使将受体的所有部分电荷都设置为零,高水密度的环形区域仍然存在。因此,在没有强吸引性溶质-溶剂相互作用的情况下,也可以在结合位点中产生局部高溶剂密度区域。