A time integration procedure for plastic deformation in elastic-viscoplastic metals

A simple unconditionally stable numerical procedure for time integration of the flow rule for large plastic deformation of an elastic-viscoplastic metal is developed. Specific attention is focused on a unified set of constitutive equations which represents a generalization (for large deformation and thermomechanical response) of the Bodner-Partom model [6, 7]. An analytical solution is obtained for large deformation simple shear at constant shear rate. Numerical examples of simple shear, a corner test exhibiting the transition from uniaxial compression to shear, and simple tension are considered which demonstrate the stability and accuracy of the procedure. It is shown that the same procedure can be used for a rate insensitive metal characterized by a yield function as well as for a rate sensitive metal characterized by an overstress model. Finally, an appendix is provided which records the basic equations associated with the small deformation theory.

[1]  P. M. Naghdi,et al.  A general theory of an elastic-plastic continuum , 1965 .

[2]  J. C. Simo,et al.  Variational and projection methods for the volume constraint in finite deformation elasto-plasticity , 1985 .

[3]  M. Rubin An elastic-viscoplastic model exhibiting continuity of solid and fluid states , 1987 .

[4]  Thomas J. R. Hughes,et al.  Unconditionally stable algorithms for quasi-static elasto/visco-plastic finite element analysis , 1978 .

[5]  P. M. Naghdi,et al.  On thermodynamics and the nature of the second law , 1977, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

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

[7]  G. Maenchen,et al.  The Tensor Code , 1963 .

[8]  Alan K. Miller,et al.  Unified constitutive equations for creep and plasticity , 1987 .

[9]  M. Rubin The significance of pure measures of distortion in nonlinear elasticity with reference to the Poynting problem , 1988 .

[10]  O. C. Zienkiewicz,et al.  The visco‐plastic approach to problems of plasticity and creep involving geometric non‐linear effects , 1978 .

[11]  P. Flory,et al.  Thermodynamic relations for high elastic materials , 1961 .

[12]  M. Rubin An Elastic-Viscoplastic Model for Metals Subjected to High Compression , 1987 .

[13]  P. Perzyna Fundamental Problems in Viscoplasticity , 1966 .

[14]  P. M. Naghdi,et al.  SOME REMARKS ON ELASTIC-PLASTIC DEFORMATION AT FINITE STRAIN , 1971 .

[15]  S. Bodner,et al.  A Large Deformation Elastic-Viscoplastic Analysis of a Thick-Walled Spherical Shell , 1972 .

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

[17]  M. Rubin An elastic-viscoplastic model for large deformation , 1986 .

[18]  Vlado A. Lubarda,et al.  A Correct Definition of Elastic and Plastic Deformation and Its Computational Significance , 1981 .

[19]  P. M. Naghdi,et al.  The significance of formulating plasticity theory with reference to loading surfaces in strain space , 1975 .

[20]  W. C. Moss,et al.  On the computational significance of the strain space formulation of plasticity theory , 1984 .

[21]  P. M. Naghdi,et al.  The second law of thermo-dynamics and cyclic processes , 1978 .

[22]  S. Bodner Review of a Unified Elastic—Viscoplastic Theory , 1987 .

[23]  S. R. Bodner,et al.  Constitutive Equations for Elastic-Viscoplastic Strain-Hardening Materials , 1975 .