For the analysis of arbitrary, by Finite Elements discretized shell structures, an efficient numerical simulation strategy with quadratic convergence including geometrically and physically nonlinear effects will be presented. In the beginning, a Finite-Rotation shell theory allowing constant shear deformations across the shell thickness is given in an isoparametric formulation. The assumed-strain concept enables the derivation of a locking-free finite element. The Layered Approach will be applied to ensure a sufficiently precise prediction of the propagation of plastic zones even throughout the shell thickness. The Riks-Wempner-Wessels global iteration scheme will be enhanced by a Line-Search procedure to ensure the tracing of nonlinear def...
In this work, a previously proposed Enhanced Assumed Strain (EAS) finite element formulation for thi...
An isogeometric thin shell formulation allowing for large-strain plastic deformation is presented. A...
The null stress (s 33 = 0) and incompressibility (J = 1) conditions in finite strain elasto-plastic ...
For the analysis of arbitrary, by Finite Elements discretized shell structures, an efficient numeric...
For the analysis of arbitrary, by Finite Elements discretized shell structures, an efficient numeric...
For the analysis of arbitrary, by Finite Elements discretized shell structures, an efficient numeric...
This work is concerned with the numerical simulation of shell structures for nonlinear elastostatics...
The geometrically-exact finite-strain variable-thickness shell model of [1] is reviewed in this pape...
A 48 degree-of-freedom doubly curved quadrilateral thin shell element, including the effect of both ...
Studying shell structures while accounting for all necessary factors is a significantly nonlinear pr...
Studying shell structures while accounting for all necessary factors is a significantly nonlinear pr...
AbstractA non-linear finite element analysis is presented, for the elasto-plastic behavior of thick ...
Studying shell structures while accounting for all necessary factors is a significantly nonlinear pr...
In this work a comparative analysis is presented between the linear and the nonlinear kinematic hard...
Modelling of structures on different scales has been a popular subject in the past. Within such a st...
In this work, a previously proposed Enhanced Assumed Strain (EAS) finite element formulation for thi...
An isogeometric thin shell formulation allowing for large-strain plastic deformation is presented. A...
The null stress (s 33 = 0) and incompressibility (J = 1) conditions in finite strain elasto-plastic ...
For the analysis of arbitrary, by Finite Elements discretized shell structures, an efficient numeric...
For the analysis of arbitrary, by Finite Elements discretized shell structures, an efficient numeric...
For the analysis of arbitrary, by Finite Elements discretized shell structures, an efficient numeric...
This work is concerned with the numerical simulation of shell structures for nonlinear elastostatics...
The geometrically-exact finite-strain variable-thickness shell model of [1] is reviewed in this pape...
A 48 degree-of-freedom doubly curved quadrilateral thin shell element, including the effect of both ...
Studying shell structures while accounting for all necessary factors is a significantly nonlinear pr...
Studying shell structures while accounting for all necessary factors is a significantly nonlinear pr...
AbstractA non-linear finite element analysis is presented, for the elasto-plastic behavior of thick ...
Studying shell structures while accounting for all necessary factors is a significantly nonlinear pr...
In this work a comparative analysis is presented between the linear and the nonlinear kinematic hard...
Modelling of structures on different scales has been a popular subject in the past. Within such a st...
In this work, a previously proposed Enhanced Assumed Strain (EAS) finite element formulation for thi...
An isogeometric thin shell formulation allowing for large-strain plastic deformation is presented. A...
The null stress (s 33 = 0) and incompressibility (J = 1) conditions in finite strain elasto-plastic ...