Families of 4-node and 9-node finite elements for a finite deformation shell theory. An assesment of hybrid stress, hybrid strain and enhanced strain elements

Abstract In this paper we discuss and compare three types of 4-node and 9-node finite elements for a recently formulated finite deformation shell theory with seven degrees of freedom. The shell theory takes thickness change into account and circumvents the use of a rotation tensor. It allows for the applicability of three-dimensional constitutive laws and equipes the configuration space with the structure of a vector space. The finite elements themselves are based either on a hybrid stress functional, on a hybrid strain functional, or on a nonlinear version of the enhanced strain concept. As independent variables either the normal and shear resultants, the strain tensor related to the deformation of the midsurface, or the incompatible enhanced strain field are taken as independent variables. The fields of equivalence of these different formulations, their limitations as well as possible improvements are discussed using different numerical examples.

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

[2]  K. Park,et al.  A Curved C0 Shell Element Based on Assumed Natural-Coordinate Strains , 1986 .

[3]  S. Lee,et al.  An eighteen‐node solid element for thin shell analysis , 1988 .

[4]  Carlo Sansour,et al.  Large viscoplastic deformations of shells. Theory and finite element formulation , 1998 .

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

[6]  S. Atluri,et al.  Formulation of a membrane finite element with drilling degrees of freedom , 1992 .

[7]  Satya N. Atluri,et al.  An analysis of, and remedies for, kinematic modes in hybrid-stress finite elements: selection of stable, invariant stress fields , 1983 .

[8]  Chahngmin Cho,et al.  An efficient assumed strain element model with six DOF per node for geometrically non‐linear shells , 1995 .

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

[10]  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.

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

[12]  K. Sze,et al.  An efficient hybrid quadrilateral Kirchhoff plate bending element , 1991 .

[13]  A. Cazzani,et al.  On some mixed finite element methods for plane membrane problems , 1997 .

[14]  S. Atluri ALTERNATE STRESS AND CONJUGATE STRAIN MEASURES, AND MIXED VARIATIONAL FORMULATIONS INVOLVING RIGID ROTATIONS, FOR COMPUTATIONAL ANALYSES OF FINITELY DEFORMED SOLIDS, WITH APPLICATION TO PLATES AND SHELLS-I , 1984 .

[15]  S. Atluri,et al.  Development and testing of stable, invariant, isoparametric curvilinear 2- and 3-D hybrid-stress elements , 1984 .

[16]  P. Pinsky,et al.  An assumed covariant strain based 9‐node shell element , 1987 .

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

[18]  H. Parisch,et al.  An investigation of a finite rotation four node assumed strain shell element , 1991 .

[19]  E. Hinton,et al.  A new nine node degenerated shell element with enhanced membrane and shear interpolation , 1986 .

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

[21]  Peter Wriggers,et al.  Theory and numerics of thin elastic shells with finite rotations , 1989 .

[22]  A. Ibrahimbegovic Stress resultant geometrically nonlinear shell theory with drilling rotations - Part I : A consistent formulation , 1994 .

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

[24]  Karl Schweizerhof,et al.  An efficient mixed hybrid 4‐node shell element with assumed stresses for membrane, bending and shear parts , 1994 .

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

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

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

[28]  J. C. Simo,et al.  On stress resultant geometrically exact shell model. Part I: formulation and optimal parametrization , 1989 .

[29]  Carlo Sansour,et al.  An exact finite rotation shell theory, its mixed variational formulation and its finite element implementation , 1992 .

[30]  Atef F. Saleeb,et al.  A hybrid/mixed model for non‐linear shell analysis and its applications to large‐rotation problems , 1990 .

[31]  Yavuz Başar,et al.  Finite-rotation shell elements for the analysis of finite-rotation shell problems , 1992 .

[32]  Carlo Sansour,et al.  The Cosserat surface as a shell model, theory and finite-element formulation , 1995 .

[33]  D. Arnold Mixed finite element methods for elliptic problems , 1990 .

[34]  F. Brezzi,et al.  A discourse on the stability conditions for mixed finite element formulations , 1990 .

[35]  F. Kollmann,et al.  Numerical analysis of viscoplastic axisymmetric shells based on a hybrid strain finite element , 1990 .

[36]  K. Wiśniewski A shell theory with independent rotations for relaxed Biot stress and right stretch strain , 1998 .

[37]  M. Chipot Finite Element Methods for Elliptic Problems , 2000 .