Variational collision integrator for polymer chains

The numerical simulation of many-particle systems (e.g. in molecular dynamics) often involves constraints of various forms. We present a symplectic integrator for mechanical systems with holonomic (bilateral) and unilateral contact constraints, the latter being in the form of a non-penetration condition. The scheme is based on a discrete variant of Hamilton's principle in which both the discrete trajectory and the unknown collision time are varied (cf. R. Fetecau, J. Marsden, M. Ortiz, M. West, Nonsmooth Lagrangian mechanics and variational collision integrators, SIAM J. Appl. Dyn. Syst. 2 (2003) 381-416]). As a consequence, the collision event enters the discrete equations of motion as an unknown that has to be computed on-the-fly whenever a collision is imminent. The additional bilateral constraints are efficiently dealt with employing a discrete null space reduction (including a projection and a local reparametrisation step) which considerably reduces the number of unknowns and improves the condition number during each time-step as compared to a standard treatment with Lagrange multipliers. We illustrate the numerical scheme with a simple example from polymer dynamics, a linear chain of beads, and test it against other standard numerical schemes for collision problems.

[1]  E. Hairer,et al.  Geometric Numerical Integration: Structure Preserving Algorithms for Ordinary Differential Equations , 2004 .

[2]  J. Marsden,et al.  Mechanical integrators derived from a discrete variational principle , 1997 .

[3]  Peter Betsch,et al.  The discrete null space method for the energy consistent integration of constrained mechanical systems. Part II: multibody dynamics , 2006 .

[4]  H. C. Andersen Rattle: A “velocity” version of the shake algorithm for molecular dynamics calculations , 1983 .

[5]  B. Leimkuhler,et al.  A molecular dynamics algorithm for mixed hard-core/continuous potentials , 2000 .

[6]  D. W. Noid Studies in Molecular Dynamics , 1976 .

[7]  Peter Betsch,et al.  The discrete null space method for the energy consistent integration of constrained mechanical systems: Part I: Holonomic constraints , 2005 .

[8]  Matthew West,et al.  Decomposition contact response (DCR) for explicit finite element dynamics , 2005, International Journal for Numerical Methods in Engineering.

[9]  Eberhard Zeidler,et al.  Applied Functional Analysis: Main Principles and Their Applications , 1995 .

[10]  Laurent O. Jay,et al.  Specialized Partitioned Additive Runge-Kutta Methods for Systems of Overdetermined DAEs with Holonomic Constraints , 2007, SIAM J. Numer. Anal..

[11]  David Chandler,et al.  Constrained impulsive molecular dynamics , 1981 .

[12]  W. Briels,et al.  Systematic coarse-graining of the dynamics of entangled polymer melts: the road from chemistry to rheology , 2011, Journal of physics. Condensed matter : an Institute of Physics journal.

[13]  J. Marsden,et al.  Discrete mechanics and variational integrators , 2001, Acta Numerica.

[14]  B. Leimkuhler,et al.  Symplectic integration of constrained Hamiltonian systems , 1994 .

[15]  Boris S. Mordukhovich,et al.  Discrete Approximations of Differential Inclusions in Infinite-Dimensional Spaces , 2005 .

[16]  Kurt Binder,et al.  Monte Carlo and Molecular Dynamics Simulations Polymer , 1995 .

[17]  B. Leimkuhler,et al.  Simulating Hamiltonian Dynamics: Hamiltonian PDEs , 2005 .

[18]  Stephen D. Bond,et al.  Stabilized Integration of Hamiltonian Systems with Hard-Sphere Inequality Constraints , 2007, SIAM J. Sci. Comput..

[19]  D. Rapaport Molecular dynamics study of a polymer chain in solution , 1979 .

[20]  S. Edwards,et al.  The Theory of Polymer Dynamics , 1986 .

[21]  Anna Walsh STUDIES IN MOLECULAR DYNAMICS , 1965 .

[22]  G. Ciccotti,et al.  Numerical Integration of the Cartesian Equations of Motion of a System with Constraints: Molecular Dynamics of n-Alkanes , 1977 .

[23]  Benedict Leimkuhler,et al.  Molecular dynamics and the accuracy of numerically computed averages , 2007, Acta Numerica.

[24]  S. Reich,et al.  Numerical methods for Hamiltonian PDEs , 2006 .

[25]  M. Karplus,et al.  Folding of a model three-helix bundle protein: a thermodynamic and kinetic analysis. , 1999, Journal of molecular biology.

[26]  Jeremy Schofield,et al.  Discontinuous molecular dynamics for semiflexible and rigid bodies. , 2006, The Journal of chemical physics.

[27]  B. Alder,et al.  Studies in Molecular Dynamics. I. General Method , 1959 .

[28]  L. Jay Beyond conventional Runge-Kutta methods in numerical integration of ODEs and DAEs by use of structures and local models , 2007 .

[29]  K. Binder Monte Carlo and molecular dynamics simulations in polymer science , 1995 .

[30]  J. Marsden,et al.  Variational integrators for constrained dynamical systems , 2008 .

[31]  H. T. Davis,et al.  Molecular dynamics study of the primitive model of 1–3 electrolyte solutions , 1990 .

[32]  S. Reich Backward Error Analysis for Numerical Integrators , 1999 .

[33]  Jerrold E. Marsden,et al.  Nonsmooth Lagrangian Mechanics and Variational Collision Integrators , 2003, SIAM J. Appl. Dyn. Syst..

[34]  J. Marsden,et al.  Asynchronous Variational Integrators , 2003 .

[35]  W. G. Madden,et al.  A new method for the molecular dynamics simulation of hard core molecules , 1982 .

[36]  A. Balakrishnan Applied Functional Analysis , 1976 .

[37]  C. W. Gear,et al.  Multirate linear multistep methods , 1984 .

[38]  Daan Frenkel,et al.  Molecular dynamics study of the dynamical properties of an assembly of infinitely thin hard rods , 1983 .

[39]  Asen L. Dontchev,et al.  Difference Methods for Differential Inclusions: A Survey , 1992, SIAM Rev..

[40]  C. Schütte,et al.  Fast simulation of polymer chains. , 2009, The Journal of chemical physics.