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EXTENDED ENSEMBLE MOLECULAR DYNAMICS METHOD FOR CONSTANT STRAIN RATE UNIAXIAL DEFORMATION OF POLYMER SYSTEMS

机译:聚合物体系的恒定应变率单轴变形的扩展分子动力学方法

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We describe a novel molecular dynamics (MD) method to simulate the uniaxial deformation of an amorphous polymer. This method is based on a rigorously defined statistical mechanics ensemble appropriate for describing an isothermal, displacement controlled, uniaxial stress mechanical test. The total number of particles is fixed and the normal stresses in the direction normal to the applied strain are constant, i.e., an NTLx sigma(yy)sigma(zz) ensemble. By using the Lagrangian of the extended system (i.e., including additional variables corresponding to the temperature and cross-sectional area fluctuations), we derive a set of equations of motion for the atomic coordinates and the additional variables appropriate to this ensemble. In order to avoid the short MD time step appropriate for the stiff covalent bonds along the polymer chains, we introduce bond length constraints. This is achieved using a variation of the commonly used SHAKE [J. P. Ryckaert, G. Ciccotti, and H. J. C. Berendsen, J. Comp. Phys. 23, 327 (1977)] algorithm. A numerical method for integrating the equations of motion with constraints via a modification of the velocity Verlet [W. C. Swope, H. C. Andersen, P. H. Berens, and K. R. Wilson, J. Chem. Phys. 76, 637 (1982)] algorithm is presented. We apply this new algorithm to the constant strain rate deformation of an amorphous polyethylene in a model containing several distinct polymer chains. To our knowledge, this is the first time that bond length constraints were applied to a macromolecular system together with an extended ensemble in which the simulation cell shape is allowed to fluctuate. (C) 1997 American Institute of Physics. [References: 18]
机译:我们描述了一种新型的分子动力学(MD)方法,以模拟非晶态聚合物的单轴变形。此方法基于严格定义的统计力学集合,适用于描述等温,位移受控的单轴应力机械测试。粒子的总数是固定的,并且在垂直于所施加应变的方向上的法向应力是恒定的,即NTLx sigma(yy)sigma(zz)系综。通过使用扩展系统的拉格朗日方程(即包括与温度和横截面积波动相对应的其他变量),我们导出了原子坐标的运动方程组和适合此集合的其他变量。为了避免适用于沿着聚合物链的刚性共价键的较短MD时间步骤,我们引入了键长约束。这是通过使用常用的SHAKE [J. P.Ryckaert,G.Ciccotti和H.J.C.Berendsen,J.Comp。物理23,327(1977)]算法。一种通过修改速度Verlet [W. C.Swope,H.C。Andersen,P.H.Berens和K.R.Wilson,J.Chem。物理76,637(1982)]算法被提出。我们将此新算法应用于包含多个不同聚合物链的模型中非晶聚乙烯的恒定应变率变形。据我们所知,这是第一次将键长约束与扩展的集合一起应用于大分子系统,在该集合中,允许模拟单元格形状发生波动。 (C)1997美国物理研究所。 [参考:18]

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