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首页> 外文期刊>Journal of chemical theory and computation: JCTC >Alchemical Free-Energy Calculations by Multiple-Replica lambda-Dynamics: The Conveyor Belt Thermodynamic Integration Scheme
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Alchemical Free-Energy Calculations by Multiple-Replica lambda-Dynamics: The Conveyor Belt Thermodynamic Integration Scheme

机译:多重复制λ动态的炼金术自由能量计算:输送带热力学集成方案

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摘要

A new method is proposed to calculate alchemical free-energy differences based on molecular dynamics (MD) simulations, called the conveyor belt thermodynamic integration CBTI) scheme. As in thermodynamic integration (TI), K replicas of the system are simulated at different values of the alchemical coupling parameter lambda. The number K is taken to be even, and the replicas are equally spaced on a forward-turn- backward-turn path, akin to a conveyor belt (CB) between the two physical end-states; and as in lambda-dynamics (AD), the lambda-values associated with the individual systems evolve in time along the simulation. However, they do so in a concerted fashion, determined by the evolution of a single dynamical variable Lambda of period 2 pi controlling the advance of the entire CB. Thus, a change of Lambda is always associated with K/2 equispaced replicas moving forward and K/2 equispaced replicas moving backward along lambda. As a result, the effective free-energy profile of the replica system along Lambda is periodic of period 27 pi K-1, and the magnitude of its variations decreases rapidly upon increasing K, at least as K-1 in the limit of large K. When a sufficient number of replicas is used, these variations become small, which enables a complete and quasi-homogeneous coverage of the lambda-range by the replica system, without application of any biasing potential. If desired, a memory-based biasing potential can still be added to further homogenize the sampling, the preoptimization of which is computationally inexpensive. The final free-energy profile along lambda is calculated similarly to TI, by binning of the Hamiltonian lambda-derivative as a function of lambda considering all replicas simultaneously, followed by quadrature integration. The associated quadrature error can be kept very low owing to the continuous and quasi-homogeneous lambda-sampling. The CBTI scheme can be viewed as a continuous/deterministic/dynamical analog of the Hamiltonian replica-exchange/permutation (HRE/HRP) schemes or as a correlated multiple-replica analog of the lambda D or lambda-local elevation umbrella sampling (lambda-LEUS) schemes. Compared to TI, it shares the advantage of the latter schemes in terms of enhanced orthogonal sampling, i.e. the availability of variable-lambda paths to circumvent conformational barriers present at specific lambda-values. Compared to HRE/HRP, it permits a deterministic and continuous sampling of the lambda-range, is expected to be less sensitive to possible artifacts of the thermo- and barostating schemes, and bypasses the need to carefully preselect a lambda-ladder and a swapping-attempt frequency. Compared to lambda-LEUS, it eliminates (or drastically reduces) the dead time associated with the preoptimization of a biasing potential. The goal of this article is to provide the mathematical/physical formulation of the proposed CBTI scheme, along with an initial application of the method to the calculation of the hydration free energy of methanol.
机译:提出了一种基于分子动力学(MD)模拟的炼金术自由能差异,称为传送带热力学积分CBTI)方案。如在热力学积分(Ti)中,在炼金术耦合参数Lambda的不同值下模拟系统的k副本。数量k均匀,复制品在向前转弯路径上同样间隔开,类似于两个物理终端状态之间的传送带(CB);与在Lambda-Dynamics(AD)中一样,与各个系统相关联的Lambda值沿着模拟在时间上发展。然而,它们以协调的方式这样做,通过控制整个CB的前进的时期2 PI的单个动态可变λ的演变来确定。因此,Lambda的变化始终与k / 2等间隔的复制品向前移动,K / 2等间化复制品沿λ向后移动。结果,沿着λ的复制系统的有效自由能曲线是周期性的27pi k-1,并且在增加k时,其变化的大小减小,至少在大k的极限中的k-1 。当使用足够数量的副本时,这些变化变小,这使得通过复制系统可以实现λ范围的完整和准均匀覆盖,而不应用任何偏置电位。如果需要,仍然可以添加基于存储基的偏置电位以进一步均匀化采样,其预曝光是计算廉价的。沿着λ的最终的自由能谱与Ti类似地计算,通过汉尔顿λ衍生物作为Lambda同时考虑所有复制品的函数,其次是正交集成。由于连续和准均匀的Lambda取样,相关的正交误差可以保持非常低。 CBTI方案可以被视为Hamilton Replica-Exchange /排列(HRE / HRE / HRP)方案的连续/确定性/动态模拟或作为Lambda D或Lambda-Location海拔伞采样的相关多重复制模拟(Lambda-雷斯)计划。与TI相比,在增强的正交采样方面,即在增强的正交采样方面,即可变Lambda路径以规避特定的λ值存在的可变λ路径的可用性。与HRE / HRP相比,它允许λ范围的确定性和连续采样,预计对热和远叠方案的可能伪像不太敏感,并且绕过需要仔细预检λ梯子和交换 - 频率。与Lambda-Leus相比,它消除了(或大幅减少)与偏置电位的偏见相关的死区时间。本文的目标是提供所提出的CBTI方案的数学/物理制定,以及初步应用该方法对甲醇的水合化能量的计算。

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