Exact integration of the von Mises elastoplasticity model with combined linear isotropic-kinematic hardening

The main purpose of this work is to present two semi-analytical solutions for the von Mises elastoplasticity model governed by combined linear isotropic-kinematic hardening. The first solution (SOLe) corresponds to strain-driven problems with constant strain rate assumption, whereas the second one (SOLσ) is proposed for stress-driven problems using constant stress rate assumption. The formulas are derived within the small strain theory Besides the new analytical solutions, a new discretized integration scheme (AMe) based on the time-continuous SOLe is also presented and the corresponding algorithmically consistent tangent tensor is provided. A main advantage of the discretized stress updating algorithm is its accuracy; it renders the exact solution if constant strain rate is assumed during the strain increment, which is a commonly adopted assumption in the standard finite element calculations. The improved accuracy of the new method (AMe) compared with the well-known radial return method (RRM) is demonstrated by evaluating two simple examples characterized by generic nonlinear strain paths.

[1]  Wai-Fah Chen,et al.  Plasticity for Structural Engineers , 1988 .

[2]  Diego Dominici NESTED DERIVATIVES: A SIMPLE METHOD FOR COMPUTING SERIES EXPANSIONS OF INVERSE FUNCTIONS , 2003 .

[3]  Ferdinando Auricchio,et al.  A novel ‘optimal’ exponential‐based integration algorithm for von‐Mises plasticity with linear hardening: Theoretical analysis on yield consistency, accuracy, convergence and numerical investigations , 2006 .

[4]  Thomas J. R. Hughes,et al.  Encyclopedia of computational mechanics , 2004 .

[5]  Mohamed Rouainia,et al.  Explicit Runge–Kutta methods for the integration of rate-type constitutive equations , 2008 .

[6]  Jean-Louis Chaboche,et al.  A review of some plasticity and viscoplasticity constitutive theories , 2008 .

[7]  K. B. Oldham,et al.  An Atlas of Functions. , 1988 .

[8]  N. Petrinic,et al.  Introduction to computational plasticity , 2005 .

[9]  Ferdinando Auricchio,et al.  On a new integration scheme for von‐Mises plasticity with linear hardening , 2003 .

[10]  Matti Ristinmaa,et al.  An alternative method for the integration of continuum damage evolution laws , 2007 .

[11]  Generalized midpoint integration algorithms for J2 plasticity with linear hardening , 2007 .

[12]  Numerical implementation of prager's kinematic hardening model in exactly integrated form for elasto-plastic analysis , 1987 .

[13]  Akhtar S. Khan,et al.  Continuum theory of plasticity , 1995 .

[14]  R. D. Krieg,et al.  Plane stress linear hardening plasticity theory , 1997 .

[15]  Jean-Philippe Ponthot,et al.  Unified stress update algorithms for the numerical simulation of large deformation elasto-plastic and elasto-viscoplastic processes , 2002 .

[16]  D. R. J. Owen,et al.  CONSISTENT LINEARIZATION FOR THE EXACT STRESS UPDATE OF PRANDTL–REUSS NON‐HARDENING ELASTOPLASTIC MODELS , 1996 .

[17]  Chein-Shan Liu A consistent numerical scheme for the von Mises mixed-hardening constitutive equations , 2004 .

[18]  S. Caddemi Computational aspects of the integration of the von Mises linear hardening constitutive laws , 1994 .

[19]  Pierre Montmitonnet,et al.  An integration scheme for Prandtl‐Reuss elastoplastic constitutive equations , 1992 .

[20]  A. Reuss,et al.  Berücksichtigung der elastischen Formänderung in der Plastizitätstheorie , 1930 .

[21]  Matti Ristinmaa,et al.  EXACT INTEGRATION OF CONSTITUTIVE EQUATIONS IN ELASTO - PLASTICITY , 1993 .

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

[23]  Giuseppe Cocchetti,et al.  A rigorous bound on error in backward-difference elastoplastic time-integration , 2003 .

[24]  R. G. Whirley,et al.  On the Numerical Implementation of Elastoplastic Models , 1984 .

[25]  H. Yu,et al.  Generalized trapezoidal numerical integration of an advanced soil model , 2008 .

[26]  László Szabó,et al.  A semi-analytical integration method for J2 flow theory of plasticity with linear isotropic hardening , 2009 .

[27]  M. Rezaiee-Pajand,et al.  On the integration schemes for Drucker–Prager's elastoplastic models based on exponential maps , 2008 .

[28]  Amir R. Khoei,et al.  On the implementation of a multi-surface kinematic hardening plasticity and its applications , 2005 .

[29]  Jean-Herve Prevost,et al.  Accurate numerical solutions for Drucker-Prager elastic-plastic models , 1986 .

[30]  Irene A. Stegun,et al.  Handbook of Mathematical Functions. , 1966 .

[31]  Kaspar Willam,et al.  On the consistency of viscoplastic formulations , 2000 .

[32]  Alf Samuelsson,et al.  Finite element analysis of elastic–plastic materials displaying mixed hardening , 1979 .

[33]  C. O. Frederick,et al.  A mathematical representation of the multiaxial Bauschinger effect , 2007 .

[34]  R. D. Krieg,et al.  Accuracies of Numerical Solution Methods for the Elastic-Perfectly Plastic Model , 1977 .

[35]  S. Mukherjee,et al.  Computational Isotropic-Workhardening Rate-Independent Elastoplasticity , 2003 .

[36]  Prandtl-Reuss elastoplasticity: On-off switch and superposition formulae , 1997 .

[37]  P. P. Lepikhin,et al.  Exact solution of problems of flow theory with isotropic-kinematic hardening. Part 1. Setting the loading trajectory in the space of stresses , 1999 .

[38]  Robert L. Taylor,et al.  Two material models for cyclic plasticity: nonlinear kinematic hardening and generalized plasticity , 1995 .

[39]  Matti Ristinmaa,et al.  Accurate stress updating algorithm based on constant strain rate assumption , 2001 .