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Computational Methods for Debonding in Composites

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270 M. Kästner et al.<br />

<strong>in</strong>clud<strong>in</strong>g problems related to distorted element shapes and poor numerical condition<br />

of the system of equations to be solved.<br />

In order to improve flexibility and efficiency of the homogenization technique<br />

an alternative modell<strong>in</strong>g strategy is exam<strong>in</strong>ed. For this purpose X-FEM – whose<br />

major benefits such as regular meshes and reduced mesh<strong>in</strong>g ef<strong>for</strong>t while reta<strong>in</strong><strong>in</strong>g all<br />

advantages of the classical f<strong>in</strong>ite element approach have been demonstrated recently<br />

[1, 6, 9, 12, 13, 16] – is applied to modell<strong>in</strong>g of composite materials here.<br />

13.2.1 Fundamentals<br />

Based on the partition of unity technique [11] X-FEM offers the possibility to model<br />

arbitrary discont<strong>in</strong>uities us<strong>in</strong>g regular f<strong>in</strong>ite element meshes that do not need to<br />

match <strong>in</strong>terfaces, a fact that is very advantageous <strong>in</strong> modell<strong>in</strong>g of cracks. Various<br />

extensions <strong>in</strong>clude enrichment functions <strong>for</strong> the crack tip [19], the application of<br />

higher order elements [15], geometrically nonl<strong>in</strong>ear <strong>for</strong>mulations [3], as well as the<br />

simulation of 3D [4, 5, 18] and bi-material cracks [17].<br />

Refer<strong>in</strong>g to textile-re<strong>in</strong><strong>for</strong>ced composites the <strong>in</strong>depence of mesh geometry and<br />

<strong>in</strong>ternal discont<strong>in</strong>uities implies that element boundaries do not con<strong>for</strong>m to a material<br />

<strong>in</strong>terface. Instead, the mechanical behaviour which is characterized by a discont<strong>in</strong>uity<br />

of stra<strong>in</strong> perpendicular to the <strong>in</strong>terface ∂G (Fig. 13.6)<br />

�<br />

˜ε1 j<br />

�<br />

˜εαβ<br />

� � �<br />

= ˜ε j1 �= 0<br />

�<br />

= 0<br />

i, j = 1,2,3; α, β = 2,3 (13.37)<br />

with ˜εij = cikc jlεkl; cij = ˜ei · e j; ˜e1 = n; [a]=a + − a − is represented by a local<br />

enrichment of the FE displacement approximation with<strong>in</strong> the element<br />

Fig. 13.6 Interface with stra<strong>in</strong><br />

discont<strong>in</strong>uity<br />

uX-FEM = ∑Niui +<br />

i<br />

� �� �<br />

∑ Nja jF<br />

j∈E<br />

� �� �<br />

FEM Enrichment<br />

(13.38)

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