Integration of self-consistent polycrystal plasticity with dislocation density based hardening laws within an implicit finite element framework: Application to low-symmetry metals

Abstract We present an implementation of the viscoplastic self-consistent (VPSC) polycrystalline model in an implicit finite element (FE) framework, which accounts for a dislocation-based hardening law for multiple slip and twinning modes at the micro-scale grain level. The model is applied to simulate the macro-scale mechanical response of a highly anisotropic low-symmetry (orthorhombic) crystal structure. In this approach, a finite element integration point represents a polycrystalline material point and the meso-scale mechanical response is obtained by the mean-field VPSC homogenization scheme. We demonstrate the accuracy of the FE-VPSC model by analyzing the mechanical response and microstructure evolution of α-uranium samples under simple compression/tension and four-point bending tests. Predictions of the FE-VPSC simulations compare favorably with experimental measurements of geometrical changes and microstructure evolution. Specifically, the model captures accurately the tension–compression asymmetry of the material associated with twinning, as well as the rigidity of the material response along the hard-to-deform crystallographic orientations.

[1]  H. J. Mcskimin,et al.  Adiabatic Elastic Moduli of Single Crystal Alpha‐Uranium , 1958 .

[2]  Surya R. Kalidindi,et al.  Representation of the orientation distribution function and computation of first-order elastic properties closures using discrete Fourier transforms , 2009 .

[3]  Gwénaëlle Proust,et al.  Modeling the effect of twinning and detwinning during strain-path changes of magnesium alloy AZ31 , 2009 .

[4]  Surya R. Kalidindi,et al.  Fast computation of first-order elastic–plastic closures for polycrystalline cubic-orthorhombic microstructures , 2007 .

[5]  L. Anand,et al.  Crystallographic texture evolution in bulk deformation processing of FCC metals , 1992 .

[6]  F. Barlat,et al.  A crystallographic dislocation model for describing hardening of polycrystals during strain path changes. Application to low carbon steels , 2013 .

[7]  C. Liu,et al.  Experimental and finite-element analysis of the anisotropic response of high-purity α-titanium in bending , 2010 .

[8]  Laurent Capolungo,et al.  Anisotropic stress–strain response and microstructure evolution of textured α-uranium , 2012 .

[9]  Surya R. Kalidindi,et al.  Building texture evolution networks for deformation processing of polycrystalline fcc metals using spectral approaches: Applications to process design for targeted performance , 2010 .

[10]  Ricardo A. Lebensohn,et al.  Modeling mechanical response and texture evolution of α-uranium as a function of strain rate and temperature using polycrystal plasticity , 2013 .

[11]  A. G. Crocker The crystallography of deformation twinning in alpha-uranium , 1965 .

[12]  E. Fisher Temperature dependence of the elastic moduli in alpha uranium single crystals, part iv (298° to 923° K) , 1966 .

[13]  Yuh J. Chao,et al.  Advances in Two-Dimensional and Three-Dimensional Computer Vision , 2000 .

[14]  Carlos N. Tomé,et al.  A dislocation-based constitutive law for pure Zr including temperature effects , 2008 .

[15]  R. Cahn Twinning and slip in α‐uranium , 1951 .

[16]  G. Proust,et al.  Modeling bending of α-titanium with embedded polycrystal plasticity in implicit finite elements , 2013 .

[17]  J. Segurado,et al.  Multiscale modeling of plasticity based on embedding the viscoplastic self-consistent formulation in implicit finite elements , 2012 .

[18]  M. Yoo Slip modes of alpha uranium , 1968 .

[19]  Surya R. Kalidindi,et al.  Deformation twinning in AZ31: Influence on strain hardening and texture evolution , 2010 .

[20]  R. A. Lebensohn,et al.  Self-consistent modelling of the mechanical behaviour of viscoplastic polycrystals incorporating intragranular field fluctuations , 2007 .

[21]  Carlos N. Tomé,et al.  Modeling Texture, Twinning and Hardening Evolution during Deformation of Hexagonal Materials , 2005 .

[22]  Surya R. Kalidindi,et al.  Delineation of first-order closures for plastic properties requiring explicit consideration of strain hardening and crystallographic texture evolution , 2008 .

[23]  S. Kalidindi,et al.  Crystal plasticity simulations using discrete Fourier transforms , 2009 .

[24]  P. Houtte,et al.  QUANTITATIVE PREDICTION OF COLD ROLLING TEXTURES IN LOW-CARBON STEEL BY MEANS OF THE LAMEL MODEL , 1999 .

[25]  Ricardo A. Lebensohn,et al.  A self-consistent anisotropic approach for the simulation of plastic deformation and texture development of polycrystals : application to zirconium alloys , 1993 .

[26]  S. Bush Uranium and Graphite , 1963 .

[27]  U. F. Kocks,et al.  Kinetics of flow and strain-hardening☆ , 1981 .

[28]  B. Lesage,et al.  The influence of temperature on slip and twinning in uranium , 1971 .

[29]  R. Cahn,et al.  Plastic deformation of alpha-uranium; twinning and slip , 1953 .

[30]  R. Mccabe,et al.  Deformation of wrought uranium: Experiments and modeling , 2010 .

[31]  S. Kalidindi,et al.  Application of microstructure sensitive design to structural components produced from hexagonal polycrystalline metals , 2008 .

[32]  R Madec,et al.  From dislocation junctions to forest hardening. , 2002, Physical review letters.