Multiscale computational homogenization methods with a gradient enhanced scheme based on the discontinuous Galerkin formulation

Abstract When considering problems of dimensions close to the characteristic length of the material, the size effects can not be neglected and the classical (so-called first-order) multiscale computational homogenization scheme (FMCH) looses accuracy, motivating the use of a second-order multiscale computational homogenization (SMCH) scheme. This second-order scheme uses the classical continuum at the micro-scale while considering a second-order continuum at the macro-scale. Although the theoretical background of the second-order continuum is increasing, the implementation into a finite element code is not straightforward because of the lack of high-order continuity of the shape functions. In this work, we propose a SMCH scheme relying on the discontinuous Galerkin (DG) method at the macro-scale, which simplifies the implementation of the method. Indeed, the DG method is a generalization of weak formulations allowing for inter-element discontinuities either at the C 0 level or at the C 1 level, and it can thus be used to constrain weakly the C 1 continuity at the macro-scale. The C 0 continuity can be either weakly constrained by using the DG method or strongly constrained by using usual C 0 displacement-based finite elements. Therefore, two formulations can be used at the macro-scale: (i) the full-discontinuous Galerkin formulation (FDG) with weak C 0 and C 1 continuity enforcements, and (ii) the enriched discontinuous Galerkin formulation (EDG) with high-order term enrichment into the conventional C 0 finite element framework. The micro-problem is formulated in terms of standard equilibrium and periodic boundary conditions. A parallel implementation in three dimensions for non-linear finite deformation problems is developed, showing that the proposed method can be integrated into conventional finite element codes in a straightforward and efficient way.

[1]  Assyr Abdulle Discontinuous Galerkin finite element heterogeneous multiscale method for elliptic problems with multiple scales , 2012, Math. Comput..

[2]  Ludovic Noels,et al.  A micro-meso-model of intra-laminar fracture in fiber-reinforced composites based on a Discontinuous Galerkin/Cohesive Zone Method , 2013 .

[3]  R. Toupin Elastic materials with couple-stresses , 1962 .

[4]  Ludovic Noels,et al.  A general discontinuous Galerkin method for finite hyperelasticity. Formulation and numerical applications , 2006 .

[5]  Fpt Frank Baaijens,et al.  An approach to micro-macro modeling of heterogeneous materials , 2001 .

[6]  A. Zervos Finite elements for elasticity with microstructure and gradient elasticity , 2008 .

[7]  Paul Steinmann,et al.  On deformational and configurational mechanics of micromorphic hyperelasticity – Theory and computation , 2007 .

[8]  T. Hughes,et al.  Continuous/discontinuous finite element approximations of fourth-order elliptic problems in structural and continuum mechanics with applications to thin beams and plates, and strain gradient elasticity , 2002 .

[9]  Georges Cailletaud,et al.  Cosserat modelling of size effects in the mechanical behaviour of polycrystals and multi-phase materials , 2000 .

[10]  Adrian J. Lew,et al.  Discontinuous Galerkin methods for non‐linear elasticity , 2006 .

[11]  Christophe Geuzaine,et al.  Imposing periodic boundary condition on arbitrary meshes by polynomial interpolation , 2012 .

[12]  B. D. Reddy,et al.  A discontinuous Galerkin formulation for classical and gradient plasticity - Part 1: Formulation and analysis , 2007 .

[13]  A. McBride,et al.  A discontinuous Galerkin formulation of a model of gradient plasticity at finite strains , 2009 .

[14]  M. Ainsworth Essential boundary conditions and multi-point constraints in finite element analysis , 2001 .

[15]  Chris J. Pearce,et al.  Scale transition and enforcement of RVE boundary conditions in second‐order computational homogenization , 2008 .

[16]  Raúl A. Feijóo,et al.  On micro‐to‐macro transitions for multi‐scale analysis of non‐linear heterogeneous materials: unified variational basis and finite element implementation , 2011 .

[17]  Paul Steinmann,et al.  Micro-to-macro transitions for heterogeneous material layers accounting for in-plane stretch , 2012 .

[18]  R. D. Mindlin Second gradient of strain and surface-tension in linear elasticity , 1965 .

[19]  J. Michel,et al.  Effective properties of composite materials with periodic microstructure : a computational approach , 1999 .

[20]  V. Kouznetsova,et al.  Multi-scale second-order computational homogenization of multi-phase materials : a nested finite element solution strategy , 2004 .

[21]  V. G. Kouznetsova,et al.  Multi-scale computational homogenization: Trends and challenges , 2010, J. Comput. Appl. Math..

[22]  Antonios Zervos,et al.  A method for creating a class of triangular C1 finite elements , 2012 .

[23]  R. D. Mindlin Micro-structure in linear elasticity , 1964 .

[24]  C. Miehe,et al.  Computational micro-to-macro transitions of discretized microstructures undergoing small strains , 2002 .

[25]  V Varvara Kouznetsova,et al.  Computational homogenization for the multi-scale analysis of multi-phase materials , 2002 .

[26]  K. Garikipati,et al.  A discontinuous Galerkin formulation for a strain gradient-dependent damage model , 2004 .

[27]  N. Aravas,et al.  Mixed finite element formulations of strain-gradient elasticity problems , 2002 .

[28]  Huajian Gao,et al.  Strain gradient plasticity , 2001 .

[29]  Christophe Geuzaine,et al.  Gmsh: A 3‐D finite element mesh generator with built‐in pre‐ and post‐processing facilities , 2009 .

[30]  Peter Hansbo,et al.  A discontinuous Galerkin method¶for the plate equation , 2002 .

[31]  R. Radovitzky,et al.  A new discontinuous Galerkin method for Kirchhoff–Love shells , 2008 .

[32]  I. Vardoulakis,et al.  A three‐dimensional C1 finite element for gradient elasticity , 2009 .

[33]  V. Kouznetsova,et al.  Multi‐scale constitutive modelling of heterogeneous materials with a gradient‐enhanced computational homogenization scheme , 2002 .

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

[35]  Assyr Abdulle,et al.  Multiscale method based on discontinuous Galerkin methods for homogenization problems , 2008 .

[36]  Rhj Ron Peerlings,et al.  Gradient enhanced damage for quasi-brittle materials , 1996 .

[37]  R. Chandran,et al.  Development of discontinuous Galerkin method for nonlocal linear elasticity , 2007 .

[38]  A. Jérusalem,et al.  A micro-model of the intra-laminar fracture in fiber-reinforced composites based on a discontinuous Galerkin/extrinsic cohesive law method , 2013 .

[39]  Christophe Geuzaine,et al.  A one field full discontinuous Galerkin method for Kirchhoff–Love shells applied to fracture mechanics , 2011 .

[40]  Christian Miehe,et al.  Strain‐driven homogenization of inelastic microstructures and composites based on an incremental variational formulation , 2002 .

[41]  N. Fleck,et al.  FINITE ELEMENTS FOR MATERIALS WITH STRAIN GRADIENT EFFECTS , 1999 .