Laboratory of Physical Chemistry, Department of Chemistry and Applied Biosciences, ETH Zürich, Vladimir-Prelog-Weg 2, 8093 Zürich, Switzerland.
J Chem Theory Comput. 2020 Apr 14;16(4):2474-2493. doi: 10.1021/acs.jctc.9b00998. Epub 2020 Mar 25.
We recently introduced a method called conveyor belt (CB) thermodynamic integration (TI) for the calculation of alchemical free-energy differences based on molecular dynamics simulations. In the present work, the CBTI approach is generalized to conformational free-energy changes, i.e., to the determination of the potential of mean force (PMF) along a conformational coordinate ξ of interest. The proposed conveyor belt umbrella sampling (CBUS) scheme relies on the parallel simulation of replicas = 0,1, ..., - 1 of the system, with even. For each replica , the instantaneous value of ξ is restrained to an anchor value . The latter anchor points are equally spaced along a forward-turn-backward-turn path (i.e., a CB) between two extreme values defining the ξ-range of interest. The rotation of the CB is controlled by a variable Λ (range from 0 to 2π) which evolves dynamically along the simulation. The evolution of Λ results from the forces exerted by the restraining potentials on the anchor points, taken equal and opposite to those they exert on the replicas. Because these forces tend to cancel out along the CB, the dynamics of Λ is essentially diffusive, and the continuous distribution of ξ-values sampled by the replica system is automatically close to homogeneous. The latter feature represents an advantage over direct counting (DCNT) and traditional umbrella sampling (TRUS), shared to some extent with replica-exchange umbrella sampling (REUS). In this work, the CBUS scheme is introduced and compared to the three latter schemes in the calculation of 45 standard absolute binding free energies. These correspond to the binding of five alkali cations to three crown ethers in three solvents. Different free-energy estimators are considered for the PMF calculation, and the calculated values are also compared to those of a previous study relying on an alchemical path, as well as to experimental data.
我们最近引入了一种称为输送带(CB)热力学积分(TI)的方法,用于根据分子动力学模拟计算炼金术自由能差。在本工作中,将 CBTI 方法推广到构象自由能变化,即确定感兴趣的构象坐标 ξ 的平均力势(PMF)。所提出的输送带伞状采样(CBUS)方案依赖于系统的 = 0,1,..., - 1 个副本的并行模拟,其中 为偶数。对于每个副本 ,将 ξ 的瞬时值约束到一个锚定值 。后者锚点沿着在两个极值定义的 ξ 范围内的前转后转路径(即 CB)均匀间隔。CB 的旋转由变量 Λ(范围从 0 到 2π)控制,该变量沿模拟动态演变。Λ 的演化来自约束势对锚点施加的力,这些力与它们对副本施加的力相等且相反。由于这些力沿 CB 趋于抵消,因此 Λ 的动力学本质上是扩散的,并且副本系统采样的 ξ 值的连续分布自动接近均匀。后一个特征相对于直接计数(DCNT)和传统伞状采样(TRUS)具有优势,在某种程度上与副本交换伞状采样(REUS)共享。在这项工作中,引入了 CBUS 方案,并在计算 45 个标准绝对结合自由能方面将其与后三个方案进行了比较。这些对应于五个碱金属阳离子在三种溶剂中与三个冠醚的结合。考虑了不同的自由能估计器来计算 PMF,并将计算值与依赖于炼金术路径的先前研究的值以及实验数据进行了比较。