Failure Predictions for DP Steel Cross-die Test using Anisotropic Damage

The Lemaitre's continuum damage model is well known in the field of damage mechanics. The anisotropic damage model given by Lemaitre is relatively simple, applicable to nonproportional loads and uses only four damage parameters. The hypothesis of strain equivalence is used to map the effective stress to the nominal stress. Both the isotropic and anisotropic damage models from Lemaitre are implemented in an in-house implicit finite element code. The damage model is coupled with an elasto-plastic material model using anisotropic plasticity (Hill-48 yield criterion) and strain-rate dependent isotropic hardening. The Lemaitre continuum damage model is based on the small strain assumption; therefore, the model is implemented in an incremental co-rotational framework to make it applicable for large strains. The damage dissipation potential was slightly adapted to incorporate a different damage evolution behavior under compression and tension. A tensile test and a low-cycle fatigue test were used to determine the damage parameters. The damage evolution was modified to incorporate strain rate sensitivity by making two of the damage parameters a function of strain rate. The model is applied to predict failure in a cross-die deep drawing process, which is well known for having a wide variety of strains and strain path changes. The failure predictions obtained from the anisotropic damage models are in good agreement with the experimental results, whereas the predictions obtained from the isotropic damage model are slightly conservative. The anisotropic damage model predicts the crack direction more accurately compared to the predictions based on principal stress directions using the isotropic damage model. The set of damage parameters, determined in a uniaxial condition, gives a good failure prediction under other triaxiality conditions.

[1]  George Z. Voyiadjis,et al.  Advances in Damage Mechanics: Metals and Metal Matrix Composites With an Introduction to Fabric Tensors , 1999 .

[2]  J. Lemaître How to use damage mechanics , 1984 .

[3]  P. Grammenoudis,et al.  Continuum Damage Models based on Energy Equivalence: Part II — Anisotropic Material Response , 2009 .

[4]  Weiyuan Zhou,et al.  Thermodynamic Significance and Basis of Damage Variables and Equivalences , 2010 .

[5]  Mgd Marc Geers,et al.  Experimental analysis of strain path dependent ductile damage mechanics and forming limits , 2009 .

[6]  R. A. Lingbeek,et al.  Tool And Blank Interaction In The Cross-Die Forming Process , 2008 .

[7]  Christophe Pinna,et al.  Local plastic strain evolution in a high strength dual-phase steel , 2010 .

[8]  J. Lemaître A CONTINUOUS DAMAGE MECHANICS MODEL FOR DUCTILE FRACTURE , 1985 .

[9]  S. Murakami,et al.  Mechanical Modeling of Material Damage , 1988 .

[10]  J. Lemaître,et al.  Engineering Damage Mechanics: Ductile, Creep, Fatigue and Brittle Failures , 2005 .

[11]  Ch. Tsakmakis,et al.  Continuum Damage Models based on Energy Equivalence: Part I — Isotropic Material Response , 2009 .

[12]  C. L. Chow,et al.  An anisotropic theory of elasticity for continuum damage mechanics , 1987 .

[13]  C. L. Chow,et al.  Anisotropic Damage-coupled Sheet Metal Forming Limit Analysis , 2009 .

[14]  George Z. Voyiadjis,et al.  A Comparative Study of Damage Variables in Continuum Damage Mechanics , 2009 .

[15]  George Z. Voyiadjis,et al.  A coupled anisotropic damage model for the inelastic response of composite materials , 2000 .

[16]  George Z. Voyiadjis,et al.  Theoretical Formulation of a Coupled Elastic—Plastic Anisotropic Damage Model for Concrete using the Strain Energy Equivalence Concept , 2009 .

[17]  Mark F. Horstemeyer,et al.  A physically motivated anisotropic tensorial representation of damage with separate functions for void nucleation, growth, and coalescence , 2007 .

[18]  C. L. Chow,et al.  Viscoplastic Constitutive Modeling of Anisotropic Damage Under Nonproportional Loading , 2001 .

[19]  Hoon Huh,et al.  Dynamic tensile characteristics of TRIP-type and DP-type steel sheets for an auto-body , 2008 .

[20]  Cemal Cem Tasan,et al.  Brittle Fracture-Based Experimental Methodology for Microstructure Analysis , 2008 .

[21]  Jpm Johan Hoefnagels,et al.  Microstructural banding effects clarified through micrographic digital image correlation , 2010 .

[22]  Wang June,et al.  An anisotropic damage criterion for deformation instability and its application to forming limit analysis of metal plates , 1985 .

[23]  D. Krajcinovic,et al.  Some fundamental issues in rate theory of damage-elastoplasticity , 1995 .

[24]  Jacques Besson,et al.  Continuum Models of Ductile Fracture: A Review , 2010 .

[25]  George Z. Voyiadjis,et al.  Damage Mechanics with Fabric Tensors , 2006 .

[26]  Wing Kam Liu,et al.  Nonlinear Finite Elements for Continua and Structures , 2000 .

[27]  J. HOL,et al.  MULTISCALE FRICTION MODELING FOR SHEET METAL FORMING , 2010 .

[28]  T. Senuma Physical Metallurgy of Modern High Strength Steel Sheets , 2001 .

[29]  C. Chow,et al.  Effect of Principal Damage Plane Rotation on Anisotropic Damage Plastic Model , 2001 .

[30]  C. L. Chow,et al.  An anisotropic theory of continuum damage mechanics for ductile fracture , 1987 .

[31]  Modeling of Anisotropic Damage for Ductile Materials in Metal Forming Processes , 2004 .

[32]  C. Chow,et al.  A Generalized Mixed Isotropic-Kinematic Hardening Plastic Model Coupled with Anisotropic Damage for Sheet Metal Forming , 2004 .

[33]  D. Krajcinovic,et al.  Introduction to continuum damage mechanics , 1986 .

[34]  C. L. Chow,et al.  On evolution laws of anisotropic damage , 1989 .

[35]  Dusan Krajcinovic,et al.  Constitutive Equations for Damaging Materials , 1983 .

[36]  J. C. Simo,et al.  Strain- and stress-based continuum damage models—I. Formulation , 1989 .