A surrogate model for computational homogenization of elastostatics at finite strain using the HDMR-based neural network approximator

We propose a surrogate model for two-scale computational homogenization of elastostatics at finite strains. The macroscopic constitutive law is made numerically available via an explicit formulation of the associated macro-energy density. This energy density is constructed by using a neural network architecture that mimics a high-dimensional model representation. The database for training this network is assembled through solving a set of microscopic boundary values problems with the prescribed macroscopic deformation gradients (input data) and subsequently retrieving the corresponding averaged energies (output data). Therefore, the two-scale computational procedure for the nonlinear elasticity can be broken down into two solvers for microscopic and macroscopic equilibrium equations that work separately in two stages, called the offline and online stages. A standard finite element method is employed to solve the equilibrium equation at the macroscale. As for mircoscopic problems, an FFT-based collocation method is applied in tandem with the Newton-Raphson iteration and the conjugate-gradient method. Particularly, we solve the microscopic equilibrium equation in the Lippmann-Schwinger form without resorting to the reference medium and thus avoid the fixed-point iteration that might require quite strict numerical stability condition in the nonlinear regime.

[1]  S. Shtrikman,et al.  A variational approach to the theory of the elastic behaviour of multiphase materials , 1963 .

[2]  J. Schröder,et al.  Computational homogenization analysis in finite plasticity Simulation of texture development in polycrystalline materials , 1999 .

[3]  Frédéric Feyel,et al.  Multiscale FE2 elastoviscoplastic analysis of composite structures , 1999 .

[4]  Julien Yvonnet,et al.  The reduced model multiscale method (R3M) for the non-linear homogenization of hyperelastic media at finite strains , 2007, J. Comput. Phys..

[5]  Marco Avellaneda,et al.  Optimal bounds and microgeometries for elastic two-phase composites , 1987 .

[6]  H. Moulinec,et al.  A fast numerical method for computing the linear and nonlinear mechanical properties of composites , 1994 .

[7]  J. Mandel,et al.  Plasticité classique et viscoplasticité , 1972 .

[8]  Jan Novák,et al.  Accelerating a FFT-based solver for numerical homogenization of periodic media by conjugate gradients , 2010, J. Comput. Phys..

[9]  J. Willis Bounds and self-consistent estimates for the overall properties of anisotropic composites , 1977 .

[10]  J. Willis,et al.  Variational Principles for Inhomogeneous Non-linear Media , 1985 .

[11]  E. Stein,et al.  Real Analysis: Measure Theory, Integration, and Hilbert Spaces , 2005 .

[12]  Pedro Ponte Castañeda The effective mechanical properties of nonlinear isotropic composites , 1991 .

[13]  Hervé Moulinec,et al.  A computational scheme for linear and non‐linear composites with arbitrary phase contrast , 2001 .

[14]  Julien Yvonnet,et al.  COMPUTATIONAL HOMOGENIZATION METHOD AND REDUCED DATABASE MODEL FOR HYPERELASTIC HETEROGENEOUS STRUCTURES , 2013 .

[15]  N. Kikuchi,et al.  Simulation of the multi-scale convergence in computational homogenization approaches , 2000 .

[16]  Koichi Yamashita,et al.  Fitting sparse multidimensional data with low-dimensional terms , 2009, Comput. Phys. Commun..

[17]  J. Willis,et al.  On the overall properties of nonlinearly viscous composites , 1988, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[18]  L. Dormieux,et al.  Combining Galerkin approximation techniques with the principle of Hashin and Shtrikman to derive a new FFT-based numerical method for the homogenization of composites , 2012 .

[19]  Geoffrey E. Hinton,et al.  Deep Learning , 2015, Nature.

[20]  R. Hill On constitutive macro-variables for heterogeneous solids at finite strain , 1972, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[21]  C. Miehe,et al.  Homogenization and multiscale stability analysis in finite magneto‐electro‐elasticity , 2015 .

[22]  Hervé Moulinec,et al.  A numerical method for computing the overall response of nonlinear composites with complex microstructure , 1998, ArXiv.

[23]  Marc‐André Keip,et al.  A multiscale FE-FFT framework for electro-active materials at finite strains , 2019, Computational Mechanics.

[24]  M. Geers,et al.  Finite strain FFT-based non-linear solvers made simple , 2016, 1603.08893.

[25]  T. Hughes,et al.  The variational multiscale method—a paradigm for computational mechanics , 1998 .

[26]  Robert D. Cook,et al.  Improved Two-Dimensional Finite Element , 1974 .

[27]  Sergei Manzhos,et al.  A random-sampling high dimensional model representation neural network for building potential energy surfaces. , 2006, The Journal of chemical physics.

[28]  J. Willis,et al.  Variational and Related Methods for the Overall Properties of Composites , 1981 .

[29]  Marc‐André Keip,et al.  A two‐scale FE‐FFT approach to nonlinear magneto‐elasticity , 2018, International Journal for Numerical Methods in Engineering.

[30]  B. A. Le,et al.  Computational homogenization of nonlinear elastic materials using neural networks , 2015 .

[31]  Felix Fritzen,et al.  Two-stage data-driven homogenization for nonlinear solids using a reduced order model , 2018 .

[32]  G. Milton The Theory of Composites , 2002 .

[33]  S. Shtrikman,et al.  A variational approach to the theory of the elastic behaviour of polycrystals , 1962 .

[34]  R. Kohn,et al.  Variational bounds on the effective moduli of anisotropic composites , 1988 .