A deformation dependent stabilization technique, exemplified by EAS elements at large strains

Abstract Stabilized finite element methods have been developed mainly in the context of Computational Fluid Dynamics (CFD) and have shown to be able to add stability to previously unstable formulations in a consistent way. In this contribution a deformation dependent stabilization technique, conceptually based on the above mentioned developments in the CFD area, is developed for Solid Mechanics to cure the well-known enhanced assumed strain (EAS) method from artificial instabilities (hourglass modes) that have been observed in the range of large compressive strains. In investigating the defect of the original formulation the dominating role of the kinematic equation as cause for the instabilities is revealed. This observation serves as key ingredient for the design of the stabilizing term, introduced on the level of the variational equation. A proper design for the stabilization parameter is given based on a mechanical interpretation of the underlying defect as well as of the stabilizing action. This stabilizing action can be thought of an additional constraint, introduced into the reparametrized Hu–Washizu functional in a least-square form, together with a deformation dependent stabilization parameter. Numerical examples show the capability of this approach to effectively eliminate spurious hourglass modes, which otherwise may appear in the presence of large compressive strains, while preserving the advantageous features of the EAS method, namely the reduction of the stiffness for an `in-plane bending' mode, i.e. when plane stress elements are used in a bending situation.

[1]  Peter Wriggers,et al.  Consistent gradient formulation for a stable enhanced strain method for large deformations , 1996 .

[2]  T. Hughes Multiscale phenomena: Green's functions, the Dirichlet-to-Neumann formulation, subgrid scale models, bubbles and the origins of stabilized methods , 1995 .

[3]  J. M. Kennedy,et al.  Hourglass control in linear and nonlinear problems , 1983 .

[4]  Thomas J. R. Hughes,et al.  Stabilization Techniques and Subgrid Scales Capturing , 1996 .

[5]  J. C. Simo,et al.  Consistent tangent operators for rate-independent elastoplasticity☆ , 1985 .

[6]  T. Hughes,et al.  A new finite element formulation for computational fluid dynamics: V. Circumventing the Babuscka-Brezzi condition: A stable Petrov-Galerkin formulation of , 1986 .

[7]  E. Ramm,et al.  Three‐dimensional extension of non‐linear shell formulation based on the enhanced assumed strain concept , 1994 .

[8]  Claes Johnson,et al.  Finite element methods for linear hyperbolic problems , 1984 .

[9]  R HughesTJ,et al.  ライスナー,ミンドリン平板理論に関する混合有限要素定式化 全高次空間の一様収束 , 1988 .

[10]  J. C. Simo,et al.  A CLASS OF MIXED ASSUMED STRAIN METHODS AND THE METHOD OF INCOMPATIBLE MODES , 1990 .

[11]  Alessandro Russo,et al.  Bubble stabilization of finite element methods for the linearized incompressible Navier-Stokes equations , 1996 .

[12]  L. Franca,et al.  Error analysis of some Galerkin least squares methods for the elasticity equations , 1991 .

[13]  Chang-Chun Wu,et al.  On optimization approaches of hybrid stress elements , 1995 .

[14]  Thomas J. R. Hughes,et al.  A mixed finite element formulation for Reissner—Mindlin plate theory: uniform convergence of all higher-order spaces , 1988 .

[15]  Ted Belytschko,et al.  Assumed strain stabilization procedure for the 9-node Lagrange shell element , 1989 .

[16]  J. C. Simo,et al.  Geometrically non‐linear enhanced strain mixed methods and the method of incompatible modes , 1992 .

[17]  F. Brezzi,et al.  On the Stabilization of Finite Element Approximations of the Stokes Equations , 1984 .

[18]  E. A. de Souza Neto,et al.  Remarks on the stability of enhanced strain elements in finite elasticity and elastoplasticity , 1995 .

[19]  Peter Wriggers,et al.  A note on enhanced strain methods for large deformations , 1996 .

[20]  Ekkehard Ramm,et al.  A class of equivalent enhanced assumed strain and hybrid stress finite elements , 1999 .

[21]  E. Stein,et al.  A 4-node finite shell element for the implementation of general hyperelastic 3D-elasticity at finite strains , 1996 .

[22]  Francisco Armero,et al.  On the formulation of enhanced strain finite elements in finite deformations , 1997 .

[23]  T. Hughes,et al.  Streamline upwind/Petrov-Galerkin formulations for convection dominated flows with particular emphasis on the incompressible Navier-Stokes equations , 1990 .

[24]  Peter M. Pinsky,et al.  Design of Galerkin generalized least squares methods for Timoshenko beams , 1996 .

[25]  T. Hughes,et al.  Two classes of mixed finite element methods , 1988 .