Chatzieleftheriou Stavros, Adendorff Matthew R, Lagaros Nikos D
Institute of Structural Analysis & Antiseismic Research, Department of Structural Engineering, School of Civil Engineering, National Technical University of Athens , 9 Heroon Polytechniou Street, Zografou Campus, GR-15780 Athens, Greece.
Laboratory of Computational Biology & Biophysics, Department of Biological Engineering, Massachusetts Institute of Technology , 77 Massachusetts Avenue, Cambridge, Massachusetts 02139-4307, United States.
J Chem Inf Model. 2016 Oct 24;56(10):1963-1978. doi: 10.1021/acs.jcim.6b00356. Epub 2016 Oct 5.
The potential energy of molecules and nanostructures is commonly calculated in the molecular mechanics formalism by superimposing bonded and nonbonded atomic energy terms, i.e. bonds between two atoms, bond angles involving three atoms, dihedral angles involving four atoms, nonbonded terms expressing the Coulomb and Lennard-Jones interactions, etc. In this work a new, generalized numerical simulation is presented for studying the mechanical behavior of three-dimensional nanostructures at the atomic scale. The energy gradient and Hessian matrix of such assemblies are usually computed numerically; a potential energy finite element model is proposed herein where these two components are expressed analytically. In particular, generalized finite elements are developed that express the interactions among atoms in a manner equivalent to that invoked in simulations performed based on the molecular dynamics method. Thus, the global tangent stiffness matrix for any nanostructure is formed as an assembly of the generalized finite elements and is directly equivalent to the Hessian matrix of the potential energy. The advantages of the proposed model are identified in terms of both accuracy and computational efficiency. In the case of popular force fields (e.g., CHARMM), the computation of the Hessian matrix by implementing the proposed method is of the same order as that of the gradient. This analysis can be used to minimize the potential energy of molecular systems under nodal loads in order to derive constitutive laws for molecular systems where the entropy and solvent effects are neglected and can be approximated as solids, such as double stranded DNA nanostructures. In this context, the sequence dependent stretch modulus for some typical base pairs step is calculated.
分子和纳米结构的势能通常在分子力学形式体系中通过叠加键合和非键合原子能量项来计算,即两个原子之间的键、涉及三个原子的键角、涉及四个原子的二面角、表示库仑和 Lennard-Jones 相互作用的非键合项等。在这项工作中,提出了一种新的广义数值模拟方法,用于研究三维纳米结构在原子尺度下的力学行为。此类组件的能量梯度和海森矩阵通常通过数值计算得到;本文提出了一种势能有限元模型,其中这两个分量通过解析方式表示。特别地,开发了广义有限元,其以与基于分子动力学方法进行的模拟中所采用的方式等效的方式来表示原子间的相互作用。因此,任何纳米结构的全局切线刚度矩阵由广义有限元组装而成,并且直接等同于势能的海森矩阵。从精度和计算效率两方面确定了所提出模型的优势。在流行的力场(例如 CHARMM)情况下,通过实施所提出的方法计算海森矩阵与计算梯度的量级相同。该分析可用于在节点载荷下最小化分子系统的势能,以便推导分子系统的本构定律,其中忽略了熵和溶剂效应,并且可以近似为固体,例如双链 DNA 纳米结构。在此背景下,计算了一些典型碱基对步长的序列依赖性拉伸模量。