Heterogeneous crystal and poly-crystal plasticity modeling from a transformation field analysis within a regularized Schmid law

The regularized Schmid law (RSL) has recently been proposed as a plastic flow criterion for poly-crystals under the crude assumptions of either uniform stress or uniform strain. We first reconsider this law for application to heterogeneous intra-crystalline plasticity, with reference to a Homogeneous Equivalent Super-Crystal. We then extend the modeling to poly-crystals with the goal to account for both stress and strain heterogeneities within as well as between grains. The transformation field analysis (TFA) is used as the homogenization procedure. This TFA is known to be accurate for materials that can be described as assemblies of plastically homogeneous domains. Otherwise, the estimates of the material effective behavior that result from its application are too stiff. Because stress and strain fields are almost everywhere uniform in laminates, we consider crystal slip organizations into multi-laminate structures. It is demonstrated that laminate layers either parallel to slip planes or normal to slip directions do not contribute to the over-stiffness due to the TFA. Thus, hierarchical multi-laminate (HML) structures are introduced where the successive laminate orientations are taken parallel to the crystal slip planes. It is shown that a conveniently weighted superposition of all the possible plane hierarchies cancels out most of the undesirable TFA contributions to the overall stiffness estimates. A relevant extension to poly-crystal plasticity of this (RSL-TFA-HML) modeling is presented.

[1]  Y. Benveniste,et al.  On transformation strains and uniform fields in multiphase elastic media , 1992, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[2]  D. Piot,et al.  A method of generating analytical yield surfaces of crystalline materials , 1996 .

[3]  W. Gambin Refined analysis of elastic-plastic crystals , 1992 .

[4]  Michael Ortiz,et al.  Nonconvex energy minimization and dislocation structures in ductile single crystals , 1999 .

[5]  K. S. Havner,et al.  On the mechanics of crystalline solids , 1973 .

[6]  P. Franciosi,et al.  Temperature and orientation dependent plasticity features of Cu and Al single crystals under axial compression-I. Lattice rotation effects and true hardening stages , 1997 .

[7]  C. Laird,et al.  Latent hardening in single crystals - I. Theory and experiments , 1991, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[8]  Laurent Stainier,et al.  A theory of subgrain dislocation structures , 2000 .

[9]  Milton Classical Hall effect in two-dimensional composites: A characterization of the set of realizable effective conductivity tensors. , 1988, Physical review. B, Condensed matter.

[10]  Véronique Favier,et al.  Micromechanical modeling of the elastic-viscoplastic behavior of polycrystalline steels having different microstructures , 2004 .

[11]  G. Dvorak Transformation field analysis of inelastic composite materials , 1992, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[12]  M. Arminjon A Regular Form of the Schmid Law. Application to the Ambiguity Problem , 1991 .

[13]  M. Berveiller,et al.  Nonlocal versus local elastoplastic behaviour of heterogeneous materials , 1993 .

[14]  Michel Bornert,et al.  An affine formulation for the prediction of the effective properties of nonlinear composites and polycrystals , 2000 .

[15]  G. Weng,et al.  A secant-viscosity approach to the time-dependent creep of an elastic viscoplastic composite , 1997 .

[16]  Pierre Suquet,et al.  Computational analysis of nonlinear composite structures using the Nonuniform Transformation Field Analysis , 2004 .

[17]  G. Lormand,et al.  Using the radon transform to solve inclusion problems in elasticity , 2004 .

[18]  E. Kröner Zur plastischen verformung des vielkristalls , 1961 .

[19]  Rodney Hill,et al.  Continuum micro-mechanics of elastoplastic polycrystals , 1965 .

[20]  P. Franciosi On flow and work hardening expression correlations in metallic single crystal plasticity , 1988 .

[21]  Amit Acharya,et al.  Lattice incompatibility and a gradient theory of crystal plasticity , 2000 .

[22]  Gilles A. Francfort,et al.  Homogenization and optimal bounds in linear elasticity , 1986 .

[23]  D Rodney,et al.  The Role of Collinear Interaction in Dislocation-Induced Hardening , 2003, Science.

[24]  J. Michel,et al.  Nonuniform transformation field analysis , 2003 .

[25]  M. Ashby,et al.  Strain gradient plasticity: Theory and experiment , 1994 .

[26]  R. Asaro,et al.  Overview no. 42 Texture development and strain hardening in rate dependent polycrystals , 1985 .

[27]  P. Franciosi,et al.  Hardening anisotropy of γγ′ superalloy single crystals—II. Numberical analysis of heterogeneity effects , 1997 .

[28]  R. Hill,et al.  XLVI. A theory of the plastic distortion of a polycrystalline aggregate under combined stresses. , 1951 .

[29]  John L. Bassani,et al.  Latent hardening in single crystals. II. Analytical characterization and predictions , 1991, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[30]  Wiktor Gambin,et al.  Model of plastic anisotropy evolution with texture-dependent yield surface , 2004 .

[31]  P. Franciosi,et al.  The concepts of latent hardening and strain hardening in metallic single crystals , 1985 .

[32]  J. D. Eshelby The determination of the elastic field of an ellipsoidal inclusion, and related problems , 1957, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[33]  Jean-Louis Chaboche,et al.  Towards a micromechanics based inelastic and damage modeling of composites , 2001 .

[34]  A. Zaoui,et al.  Crystal hardening and the issue of uniqueness , 1989 .

[35]  M. Berveiller,et al.  A new class of micro–macro models for elastic–viscoplastic heterogeneous materials , 2002 .

[36]  Mitchell Luskin,et al.  Approximation of a laminated microstructure for a rotationally invariant, double well energy density , 1996 .

[37]  D. Kuhlmann-wilsdorf Why do dislocations assemble into interfaces in epitaxy as well as in crystal plasticity? To minimize free energy , 2002 .

[38]  J. Berryman Bounds on elastic constants for random polycrystals of laminates , 2004 .

[39]  J. Willis,et al.  The effect of spatial distribution on the effective behavior of composite materials and cracked media , 1995 .

[40]  Jacob Fish,et al.  Finite deformation plasticity for composite structures: Computational models and adaptive strategies , 1999 .

[41]  P. Dawson,et al.  Mesoscale Modeling of Microstructure and Texture Evolution During Deformation Processing of Metals , 2002 .

[42]  J. Rice,et al.  Constitutive analysis of elastic-plastic crystals at arbitrary strain , 1972 .