HERK integration of finite-strain fully anisotropic plasticity models

Abstract For finite strain plasticity, we use the multiplicative decomposition of the deformation gradient to obtain a differential-algebraic system (DAE) in the semi-explicit form and solve it by a half-explicit algorithm. The terminology HERK is synonym of Half-Explicit Runge-Kutta method for DAE. The source is here the right Cauchy-Green tensor and an exact Jacobian of the second Piola-Kirchhoff stress is determined with respect to this source. The system is composed by a smooth nonlinear first-order differential equation and a non-smooth algebraic equation. The development of a half-explicit constitutive integrator is the content of this work. The integration makes use of an explicit Runge-Kutta method for the flow law complemented by the yield constraint. The flow law is a first-order differential equation and the yield constraint (including the loading/unloading conditions) is seen as the invariant of system. A half-explicit method is adopted to ensure satisfaction of the invariant. The resulting scalar equation is solved by the Newton-Raphson method to obtain the plastic multiplier. We make use of the elastic Mandel stress construction, which is power-consistent with the plastic strain rate. Iso-error maps are presented for a combination of Neo-Hookean material using the Hill yield criterion and a associative flow law. Two complete numerical examples are presented.

[1]  J. C. Simo,et al.  Algorithms for static and dynamic multiplicative plasticity that preserve the classical return mapping schemes of the infinitesimal theory , 1992 .

[2]  E. Hairer,et al.  Half-explicit Runge-Kutta methods for differential-algebraic systems of index 2 , 1993 .

[3]  Robert L. Taylor,et al.  Improved versions of assumed enhanced strain tri-linear elements for 3D finite deformation problems☆ , 1993 .

[4]  P. Areias,et al.  Finite element formulation for modeling nonlinear viscoelastic elastomers , 2008 .

[5]  A. A. Fernandes,et al.  Analysis of 3D problems using a new enhanced strain hexahedral element , 2003 .

[6]  E. Kröner,et al.  Allgemeine Kontinuumstheorie der Versetzungen und Eigenspannungen , 1959 .

[7]  Peter Betsch,et al.  Numerical implementation of multiplicative elasto-plasticity into assumed strain elements with application to shells at large strains , 1999 .

[8]  L. Petzold Order results for implicit Runge-Kutta methods applied to differential/algebraic systems , 1986 .

[9]  En-Jui Lee Elastic-Plastic Deformation at Finite Strains , 1969 .

[10]  Ernst Hairer,et al.  Symmetrized half-explicit methods for constrained mechanical systems , 1993 .

[11]  P. Wriggers Nonlinear Finite Element Methods , 2008 .

[12]  M. Arnold Half-explicit Runge-Kutta methods with explicit stages for differential-algebraic systems of index 2 , 1998 .

[13]  J. Mandel,et al.  Equations constitutives et directeurs dans les milieux plastiques et viscoplastiques , 1973 .

[14]  J. C. Simo,et al.  A framework for finite strain elastoplasticity based on maximum plastic dissipation and the multiplicative decomposition. part II: computational aspects , 1988 .

[15]  J. I. Barbosa,et al.  A new semi-implicit formulation for multiple-surface flow rules in multiplicative plasticity , 2012 .

[16]  Ekkehard Ramm,et al.  EAS‐elements for two‐dimensional, three‐dimensional, plate and shell structures and their equivalence to HR‐elements , 1993 .

[17]  P. Deuflhard,et al.  One-step and extrapolation methods for differential-algebraic systems , 1987 .

[18]  R. D. Wood,et al.  Nonlinear Continuum Mechanics for Finite Element Analysis , 1997 .

[19]  Joze Korelc,et al.  Multi-language and Multi-environment Generation of Nonlinear Finite Element Codes , 2002, Engineering with Computers.

[20]  E. Ramm,et al.  Three‐dimensional extension of non‐linear shell formulation based on the enhanced assumed strain concept , 1994 .

[21]  Uri M. Ascher,et al.  Sequential Regularization Methods for Higher Index DAEs with Constraint Singularities: The Linear Index-2 Case , 1996 .

[22]  Jeremiah G Murphy,et al.  Transversely isotropic biological, soft tissue must be modelled using both anisotropic invariants , 2013 .

[23]  F. Gruttmann,et al.  Elastoplastic orthotropy at finite strains: multiplicative formulation and numerical implementation , 2003 .

[24]  S. Nemat-Nasser Plasticity: A Treatise on Finite Deformation of Heterogeneous Inelastic Materials , 2004 .

[25]  J. C. Simo,et al.  A CLASS OF MIXED ASSUMED STRAIN METHODS AND THE METHOD OF INCOMPATIBLE MODES , 1990 .

[26]  A large-deformation multiplicative framework for anisotropic elastoplastic materialswith application to sheet metal forming , 2010 .

[27]  M. Ortiz,et al.  Formulation of implicit finite element methods for multiplicative finite deformation plasticity , 1990 .

[28]  E. H. Lee,et al.  Finite‐Strain Elastic—Plastic Theory with Application to Plane‐Wave Analysis , 1967 .

[29]  Michael Ortiz,et al.  A unified approach to finite deformation elastoplastic analysis based on the use of hyperelastic constitutive equations , 1985 .