Department of Bioengineering, Clemson University, Clemson, South Carolina 29634, USA.
Biointerphases. 2009 Dec;4(4):57-64. doi: 10.1116/1.3266417.
The simulation of the interactions of proteins with charged surfaces in a condensed-phase aqueous solution containing electrolytes using empirical force field based methods is predominantly governed by nonbonded interactions between the atoms of the protein, surface, and the solvent. Electrostatic effects represent the strongest type of these interactions and the type that is most difficult to accurately represent because of their long-range influence. While many different methods have been developed to represent electrostatic interactions, the particle mesh Ewald summation (PME) method is generally considered to be the most accurate one for calculating these effects. However, the PME method was designed for systems with three-dimensional (3D) periodicity, and not for interfacial systems such as the case of protein adsorption to a charged surface. Interfacial systems such as these have only two-dimensional periodicity, which may not be appropriate for treatment with PME due to the possibility that the presence of multiple charged image surfaces parallel to the primary simulation cell's surface, may introduce nonphysical effects on the behavior of the charged molecules in the system. In an effort to address this issue, the authors have conducted a set of nanosecond-scale molecular dynamics simulations to calculate the equilibrium distribution of Na(+) and Cl(-) ions near a charged surface using PME and a range of radial cutoff methods for treating electrostatic interactions, where the cutoffs prevent interaction with the periodic images of the system. The resulting ion concentration profiles were compared to one another and to a continuum analytical solution of the theoretical ion distribution obtained from the Poisson-Boltzmann equation. Their results show that the PME method does not introduce the suspected nonphysical effects in the ion distributions due to the 3D periodic images of the system, thus indicating that it is appropriate for use for this type of molecular simulation. Although their interest is motivated by protein-surface interactions, the conclusions are applicable for the treatment of electrostatics in other aqueous systems with two-dimensional periodicity.
使用基于经验力场的方法模拟蛋白质与含有电解质的凝聚相水溶液中带电表面的相互作用,主要由蛋白质、表面和溶剂原子之间的非键相互作用控制。静电相互作用代表了这些相互作用中最强的类型,也是最难准确表示的类型,因为它们具有远程影响。尽管已经开发了许多不同的方法来表示静电相互作用,但粒子网格 Ewald 求和 (PME) 方法通常被认为是计算这些效应最准确的方法。然而,PME 方法是为具有三维 (3D) 周期性的系统设计的,而不是为界面系统设计的,例如蛋白质吸附到带电表面的情况。像这样的界面系统只有二维周期性,由于多个带电荷的镜像表面平行于主模拟单元表面的存在,可能会对系统中带电分子的行为产生非物理效应,因此可能不适合使用 PME 进行处理。为了解决这个问题,作者进行了一系列纳秒尺度的分子动力学模拟,使用 PME 和一系列处理静电相互作用的径向截止方法来计算带电表面附近 Na(+) 和 Cl(-) 离子的平衡分布,其中截止防止与系统的周期性镜像相互作用。将得到的离子浓度分布曲线相互比较,并与从泊松-玻尔兹曼方程获得的理论离子分布的连续分析解进行比较。他们的结果表明,PME 方法不会由于系统的 3D 周期性镜像而在离子分布中引入可疑的非物理效应,因此表明它适合用于这种类型的分子模拟。尽管他们的兴趣是由蛋白质-表面相互作用引起的,但这些结论适用于具有二维周期性的其他含水系统中静电的处理。