An improved EAS brick element for finite deformation

A new enhanced assumed strain brick element for finite deformations in finite elasticity and plasticity is presented. The element is based on an expansion of shape function derivatives using Taylor series and an extended set of orthogonality conditions that have to be satisfied for an hourglassing free EAS formulation. Such approach has not been applied so far in the context of large deformation three-dimensional problems. It leads to a surprisingly well-behaved locking and hourglassing free element formulation. Major advantage of the new element is its shear locking free performance in the limit of very thin elements, thus it is applicable to shell type problems. Crucial for the derivation of the residual and consistent tangent matrix of the element is the automation of the implementation by automatic code generation.

[1]  R. L. Harder,et al.  A proposed standard set of problems to test finite element accuracy , 1985 .

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

[3]  Peter Wriggers,et al.  A stabilization technique to avoid hourglassing in finite elasticity , 2000 .

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

[5]  Klaus-Jürgen Bathe,et al.  On the stability of mixed finite elements in large strain analysis of incompressible solids , 1997 .

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

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

[8]  Francisco Armero,et al.  On the locking and stability of finite elements in finite deformation plane strain problems , 2000 .

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

[10]  Jože Korelc,et al.  Automation of primal and sensitivity analysis of transient coupled problems , 2009 .

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

[12]  Peter Wriggers,et al.  A finite deformation brick element with inhomogeneous mode enhancement , 2009 .

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

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

[15]  S. Reese On a physically stabilized one point finite element formulation for three-dimensional finite elasto-plasticity , 2005 .

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

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

[18]  J. C. Simo,et al.  On a stress resultant geometrically exact shell model. Part II: the linear theory; computational aspects , 1989 .

[19]  Peter Wriggers,et al.  An efficient 3D enhanced strain element with Taylor expansion of the shape functions , 1996 .

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

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

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

[23]  P. Wriggers Nonlinear Finite Element Methods , 2008 .

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