Discontinuous Displacement Approximation for Capturing Plastic Localization

It is proposed to capture localized plastic deformation via the inclusion of regularized displacement discontinuities at element boundaries (interfaces) of the finite element subdivision. The regularization is based on a kinematic assumption for an interface that resembles that which is pertinent to the classical shear band concept. As a by-product of the regularization, an intrinsic band width is introduced as a ‘constitutive’ property rather than a geometric feature of the finite element mesh. In this way the spurious mesh sensitivity, which is obtained when the displacement approximation is continuous, can be avoided. Another consequence is that the interfacial relation between the elements is derived directly from the conventional constitutive properties of the continuously deforming material. An interesting feature is that the acoustic tensor will not only play a role for diagnosing discontinuous bifurcation but will also serve as the tangent stiffness tensor of the interface (up to within a scalar factor). An analytical investigation of the behaviour of the interface is carried out and it is shown that dilatation may indeed accompany slip within a ‘shear’ band for a general plasticity model. The significance of proper mesh alignment is demonstrated for a simple problem in plane strain and plane stress. It is shown that a unique structural post-peak response (in accordance with non-linear fracture mechanics) can be achieved when the plastic softening modulus is properly related to the bandwidth. The paper concludes with a numerical simulation of the gradual development of a shear band in a soil slope.

[1]  R. Hill Acceleration waves in solids , 1962 .

[2]  Richard Bellman,et al.  Plastic Flow and Fracture in Solids , 1962 .

[3]  N. S. Ottosen,et al.  Properties of discontinuous bifurcation solutions in elasto-plasticity , 1991 .

[4]  Zenon Mróz,et al.  Finite element analysis of deformation of strain‐softening materials , 1981 .

[5]  J. Mandel Conditions de Stabilité et Postulat de Drucker , 1966 .

[6]  M. Ortiz,et al.  A finite element method for localized failure analysis , 1987 .

[7]  Ola Dahlblom,et al.  Smeared Crack Analysis Using Generalized Fictitious Crack Model , 1990 .

[8]  A. Hillerborg,et al.  Analysis of crack formation and crack growth in concrete by means of fracture mechanics and finite elements , 1976 .

[9]  J. Rice Localization of plastic deformation , 1976 .

[10]  Kenneth Runesson,et al.  Discontinuous bifurcations of elastic-plastic solutions at plane stress and plane strain , 1991 .

[11]  T. Belytschko,et al.  A finite element with embedded localization zones , 1988 .

[12]  C. R. Johnson,et al.  A Finite Element Method for Problems in Perfect Plasticity Using Discontinuous Trial Functions , 1981 .

[13]  R. Larsson,et al.  Numerical simulation of plastic localization , 1990 .

[14]  Z. Bažant Mechanics of Distributed Cracking , 1986 .

[15]  R. Borst,et al.  Localisation in a Cosserat continuum under static and dynamic loading conditions , 1991 .

[16]  Niels Saabye Ottosen,et al.  Thermodynamic Consequences of Strain Softening in Tension , 1986 .

[17]  E. Dvorkin,et al.  Finite elements with displacement interpolated embedded localization lines insensitive to mesh size and distortions , 1990 .

[18]  K. Runesson,et al.  Finite element simulation of localized plastic deformation , 1991 .

[19]  Characteristics and Computational Procedure in Softening Plasticity , 1989 .

[20]  J. Rice,et al.  CONDITIONS FOR THE LOCALIZATION OF DEFORMATION IN PRESSURE-SENSITIVE DILATANT MATERIALS , 1975 .

[21]  I. Vardoulakis,et al.  The thickness of shear bands in granular materials , 1987 .

[22]  M. Klisinski,et al.  FINITE ELEMENT WITH INNER SOFTENING BAND , 1991 .