Time integration in the context of energy control and locking free finite elements

SummaryIn the present paper two main research areas of computational mechanics, namely the finite element development and the design of time integration algorithms are reviewed and discussed with a special emphasis on their combination. The finite element techniques are designed to prevent locking and the time integration schemes to guarantee numerical stability in non-linear elastodynamics. If classical finite element techniques are used, their combination with time integration schemes allow to avoid any modifications on the element or algorithmic level. It is pointed out, that on the other hand Assumed Stress and Enhanced Assumed Strain elements have to be modified if they are combined with energy conserving or decaying time integration schemes, especially the Energy-Momentum Method in its original and generalized form. The paper focusses on the necessary algorithmic formulation of Enhanced Assumed Strain elements which will be developed by the reformulation of the Generalized Energy-Momentum Method based on a classical one-field functional, the extension to a modifiedHu-Washizu three-field functional including enhanced strains and a suitable time discretization of the additional strain terms. The proposed method is applied to non-linear shell dynamics using a shell element which allows for shear deformation and thickness change, and in which the Enhanced Assumed Strain Concept is introduced to avoid artificial thickness locking. Selected examples illustrate the locking free and numerically stable analysis.

[1]  J. C. Simo,et al.  The discrete energy-momentum method. Conserving algorithms for nonlinear elastodynamics , 1992 .

[2]  J. C. Simo,et al.  A new energy and momentum conserving algorithm for the non‐linear dynamics of shells , 1994 .

[3]  J. C. Simo,et al.  Non-linear dynamics of three-dimensional rods: Exact energy and momentum conserving algorithms , 1995 .

[4]  Sven Klinkel,et al.  A geometrical non‐linear brick element based on the EAS‐method , 1997 .

[5]  Theodore H. H. Pian,et al.  Alternative ways for formulation of hybrid stress elements , 1982 .

[6]  On the equivalence of non-conforming element and hybrid stress element , 1982 .

[7]  J. Z. Zhu,et al.  The finite element method , 1977 .

[8]  K. Schweizerhof,et al.  On a systematic development of trilinear three-dimensional solid elements based on Simo's enhanced strain formulation , 1996 .

[9]  Peter Betsch,et al.  A nonlinear extensible 4-node shell element based on continuum theory and assumed strain interpolations , 1996 .

[10]  O. C. Zienkiewicz,et al.  An alpha modification of Newmark's method , 1980 .

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

[12]  Robert Eberlein Finite-Elemente-Konzepte für Schalen mit großen elastischen und plastischen Verzerrungen , 1997 .

[13]  Robert L. Taylor,et al.  A Quadrilateral Mixed Finite Element with Two Enhanced Strain Modes , 1995 .

[14]  Ekkehard Ramm,et al.  EAS‐elements for two‐dimensional, three‐dimensional, plate and shell structures and their equivalence to HR‐elements , 1993 .

[15]  Boštjan Brank,et al.  ON NON-LINEAR DYNAMICS OF SHELLS: IMPLEMENTATION OF ENERGY-MOMENTUM CONSERVING ALGORITHM FOR A FINITE ROTATION SHELL MODEL , 1998 .

[16]  Thomas J. R. Hughes,et al.  FINITE-ELEMENT METHODS FOR NONLINEAR ELASTODYNAMICS WHICH CONSERVE ENERGY. , 1978 .

[17]  Cv Clemens Verhoosel,et al.  Non-Linear Finite Element Analysis of Solids and Structures , 1991 .

[18]  K. Bathe,et al.  A four‐node plate bending element based on Mindlin/Reissner plate theory and a mixed interpolation , 1985 .

[19]  Byung Chai Lee,et al.  EQUIVALENCE BETWEEN ENHANCED ASSUMED STRAIN METHOD AND ASSUMED STRESS HYBRID METHOD BASED ON THE HELLINGER–REISSNER PRINCIPLE , 1996 .

[20]  Carlo Sansour,et al.  On hybrid stress, hybrid strain and enhanced strain finite element formulations for a geometrically exact shell theory with drilling degrees of freedom , 1998 .

[21]  K. Bathe,et al.  A continuum mechanics based four‐node shell element for general non‐linear analysis , 1984 .

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

[23]  J. C. Simo,et al.  Stability and convergence of a class of enhanced strain methods , 1995 .

[24]  M. A. Crisfield,et al.  Non-Linear Finite Element Analysis of Solids and Structures: Advanced Topics , 1997 .

[25]  T. Pian,et al.  Rational approach for assumed stress finite elements , 1984 .

[26]  M. Crisfield,et al.  Non‐Linear Finite Element Analysis of Solids and Structures, Volume 1 , 1993 .

[27]  Y. Başar,et al.  Large inelastic strain analysis by multilayer shell elements , 2000 .

[28]  Peter Wriggers,et al.  Finite element concepts for finite elastoplastic strains and isotropic stress response in shells: theoretical and computational analysis , 1999 .

[29]  U. Galvanetto,et al.  AN ENERGY‐CONSERVING CO‐ROTATIONAL PROCEDURE FOR THE DYNAMICS OF PLANAR BEAM STRUCTURES , 1996 .

[30]  Peter Wriggers,et al.  IMPROVED ENHANCED STRAIN FOUR-NODE ELEMENT WITH TAYLOR EXPANSION OF THE SHAPE FUNCTIONS , 1997 .

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

[32]  Ekkehard Ramm,et al.  Nonlinear shell formulations for complete three-dimensional constitutive laws including composites and laminates , 1994 .

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

[34]  Xikui Li,et al.  MIXED STRAIN ELEMENTS FOR NON‐LINEAR ANALYSIS , 1993 .

[35]  Barna A. Szabó,et al.  Hierarchic plate and shell models based on p-extension , 1988 .

[36]  Carlo Sansour,et al.  A theory and finite element formulation of shells at finite deformations involving thickness change: Circumventing the use of a rotation tensor , 1995, Archive of Applied Mechanics.

[37]  E. Stein,et al.  An assumed strain approach avoiding artificial thickness straining for a non‐linear 4‐node shell element , 1995 .

[38]  Ekkehard Ramm,et al.  Generalized Energy–Momentum Method for non-linear adaptive shell dynamics , 1999 .

[39]  Robert L. Taylor,et al.  Improved versions of assumed enhanced strain tri-linear elements for 3D finite deformation problems☆ , 1993 .

[40]  T. Hughes,et al.  Finite Elements Based Upon Mindlin Plate Theory With Particular Reference to the Four-Node Bilinear Isoparametric Element , 1981 .

[41]  C. Schwab P- and hp- finite element methods : theory and applications in solid and fluid mechanics , 1998 .

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

[43]  Edward L. Wilson,et al.  Incompatible Displacement Models , 1973 .

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

[45]  M. Crisfield,et al.  Dynamics of 3-D co-rotational beams , 1997 .

[46]  D. Braess Enhanced assumed strain elements and locking in membrane problems , 1998 .

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

[48]  O. C. Zienkiewicz,et al.  Reduced integration technique in general analysis of plates and shells , 1971 .

[49]  E. Ramm,et al.  Shear deformable shell elements for large strains and rotations , 1997 .

[50]  J. C. Simo,et al.  On the Variational Foundations of Assumed Strain Methods , 1986 .

[51]  Dr.-Ing. C. Sansour A Theory and finite element formulation of shells at finite deformations involving thickness change , 1995 .

[52]  J. C. Nagtegaal,et al.  Using assumed enhanced strain elements for large compressive deformation , 1996 .

[53]  Christian Miehe,et al.  A theoretical and computational model for isotropic elastoplastic stress analysis in shells at large strains , 1998 .

[54]  M. Crisfield,et al.  Energy‐conserving and decaying Algorithms in non‐linear structural dynamics , 1999 .

[55]  S. Timoshenko,et al.  THEORY OF PLATES AND SHELLS , 1959 .

[56]  M. Crisfield,et al.  An energy conserving co-rotational procedure for non-linear dynamics with finite elements , 1996 .

[57]  Ekkehard Ramm,et al.  Constraint Energy Momentum Algorithm and its application to non-linear dynamics of shells , 1996 .

[58]  R. Hauptmann,et al.  A SYSTEMATIC DEVELOPMENT OF 'SOLID-SHELL' ELEMENT FORMULATIONS FOR LINEAR AND NON-LINEAR ANALYSES EMPLOYING ONLY DISPLACEMENT DEGREES OF FREEDOM , 1998 .

[59]  J. C. Simo,et al.  On a stress resultant geometrically exact shell model. Part VI: Conserving algorithms for non‐linear dynamics , 1992 .

[60]  E. Wilson,et al.  A non-conforming element for stress analysis , 1976 .

[61]  Sven Klinkel,et al.  A continuum based three-dimensional shell element for laminated structures , 1999 .

[62]  Thomas J. R. Hughes,et al.  Improved numerical dissipation for time integration algorithms in structural dynamics , 1977 .

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

[64]  T. Pian Derivation of element stiffness matrices by assumed stress distributions , 1964 .

[65]  Peter Wriggers,et al.  On enhanced strain methods for small and finite deformations of solids , 1996 .

[66]  Nathan M. Newmark,et al.  A Method of Computation for Structural Dynamics , 1959 .

[67]  Ernst Rank,et al.  On the accuracy of p-version elements for the Reissner-Mindlin plate problem , 1998 .

[68]  Peter Wriggers,et al.  Nonlinear Dynamics of Shells: Theory, Finite Element Formulation, and Integration Schemes , 1997 .

[69]  Jintai Chung,et al.  A Time Integration Algorithm for Structural Dynamics With Improved Numerical Dissipation: The Generalized-α Method , 1993 .

[70]  S. Reese,et al.  A comparison of three-dimensional continuum and shell elements for finite plasticity , 1996 .

[71]  Robert L. Taylor,et al.  A systematic construction of B‐bar functions for linear and non‐linear mixed‐enhanced finite elements for plane elasticity problems , 1999 .

[72]  Y. Başar,et al.  Finite-rotation theories for composite laminates , 1993 .

[73]  E. Ramm,et al.  Large elasto-plastic finite element analysis of solids and shells with the enhanced assumed strain concept , 1996 .

[74]  F. Armero,et al.  Formulation and analysis of conserving algorithms for frictionless dynamic contact/impact problems , 1998 .

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

[76]  Carlo Sansour,et al.  Large strain deformations of elastic shells constitutive modelling and finite element analysis , 1998 .