• Aucun résultat trouvé

Combescure Smooth nodal stresses in the XFEM for crack propagation simulations X

N/A
N/A
Protected

Academic year: 2021

Partager "Combescure Smooth nodal stresses in the XFEM for crack propagation simulations X"

Copied!
1
0
0

Texte intégral

(1)

International Conference on Extended Finite Element Methods - XFEM 2013 September 11 – 13, 2013, Lyon, France A. Gravouil, Y. Renard and A. Combescure

Smooth nodal stresses in the XFEM for crack propagation simulations

X. Peng, S. P. A. Bordas

Institute of mechanics and Advanced materials, Cardiff University, CF24 3AA, Cardiff, UK BordasS@cardiff.ac.uk

S. Natarajan

School of Civil and Environmental Engineering, The University of New South Wales, Sydney, Australia

Key Words:twice-interpolating approximation, high order element, smooth nodal stress, extended finite element method, crack propagation.

ABSTRACT

In this paper, we present a method to achieve smooth nodal stresses in the XFEM without post- processing. This method was developed by borrowing the ideas from the “twice interpolating approxi- mations” (TFEM) [1]. The salient feature of the method is to introduce an “average” gradient into the construction of the approximation, resulting in improved solution accuracy, both in the vicinity of the crack tip and in the far field. Due to the higher order polynomial basis provided by the interpolants, the new approximation enhances the smoothness of the solution without requiring an increased number of degrees of freedom. This is particularly advantageous for low-order elements and in fracture mechan- ics, where smooth stresses are important when maximum principal stress is used as crack propagation criteria. Since the new approach adopts the same mesh discretization, i.e. simplex meshes, it can be easily extended to various problems and is easily implemented.

We discuss the increase in the bandwidth which is a major drawback of the present method and can be alleviated by using an element-by-element solution strategy. Numerical tests show that the new method is as robust as the XFEM, considering precision, model size and post-processing time. By comparing the results from the present method with the XFEM for crack propagation in homogeneous material, we conclude that for two-dimensional problems, the proposed method tends to be an efficient alternative to the classical XFEM [2,3] especially when local, stress-based propagation criteria is used.

REFERENCES

[1] C. Zheng, S. C. Wu, X. H. Tang and J. H. Zhang. A novel twice interpolation for solid me- chanics problems.Acta Mech. Sin., Vol.26(2), 265–278, 2011.

[2] T. Black, and T. Belytschko. Elastic crack growth in finite elements with minimal remeshing.

Int. J. Numer. Meth. Engng., Vol.45, 601–620, 1999.

[3] N. Mo¨es, J. Dolbow and T. Belytschko. A finite element method for crack growth without remeshing.Int. J. Numer. Meth. Engng., Vol.46, 135–150, 1999.

Références

Documents relatifs

In this work, a new formulation is developed within the phase field method for modeling stress corrosion cracking induced by anodic dissolution.. The effects of both

Keywords: adaptivity, coarse graining, extended brdging scale method, virtual atom cluster model, extended finite element methods, molecular statics, multiscale methods,

Then, from the knowledge of the elastic parameters, of the fracture resistance and of the regularization parameter of the phase field method, essentially iden- tified from

growth in linear elastic fracture using XFEM 25 Danas Sutula

Three-Dimensional Crack Propagation with Global Enrichment XFEM and Vector Level SetsK.

The fictitious domain approach we implement is inspired by the eXtended Finite Element Method (XFEM) [23], since it consists partially in cutting the basis functions near or around

In Figure 4, we have plotted the energy transfer ratio - when the wave passes from the finite element to the molecular domain - as a function of the number of atoms involved in

This manuscript furthers along this line and combines molecular dynam- ics for modelling the fracture process at the crack tip with an extended finite element method (XFEM), where