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Computational Methods for Debonding in Composites

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120 X. Martínez et al.<br />

6.1 Introduction<br />

The use of new materials <strong>in</strong> structural applications implies deal<strong>in</strong>g with new failure<br />

processes, not exist<strong>in</strong>g <strong>in</strong> traditional materials. One of these is the delam<strong>in</strong>ation<br />

phenomenon found <strong>in</strong> lam<strong>in</strong>ated composites. The lost of adherence between the<br />

different layers of the composite leads to a reduction of the section strength and<br />

stiffness that can f<strong>in</strong>ish <strong>in</strong> a structural failure.<br />

The importance of this phenomenon is demonstrated by the amount of authors<br />

that have developed theories and <strong>for</strong>mulations to deal with it. All authors that have<br />

studied the problem agree that the delam<strong>in</strong>ation process is characterized by two<br />

ma<strong>in</strong> phenomenons, the crack <strong>in</strong>itiation and its propagation along the composite.<br />

Crack <strong>in</strong>itiation can be obta<strong>in</strong>ed by compar<strong>in</strong>g the stra<strong>in</strong>–stress state of the material,<br />

<strong>in</strong> the region where delam<strong>in</strong>ation takes place, with a critical one [1, 4, 6, 15] or <strong>in</strong><br />

terms of the traction versus relative displacement [2, 3, 12]. And the delam<strong>in</strong>ation<br />

propagation is usually treated open<strong>in</strong>g the mesh to simulate the crack effect where it<br />

takes place. To open the mesh different procedures are proposed. One of them is the<br />

virtual crack closure technique (VCCT) [8], based on the assumption that when a<br />

crack is extended, the energy required to open the crack is the same required to close<br />

it. Another procedure, each time more used, is the use of a cohesive zone model [4].<br />

The cohesion elements are placed <strong>in</strong> the <strong>in</strong>terface of the layers that can suffer delam<strong>in</strong>ation<br />

and its propagation is obta<strong>in</strong>ed with damage or plastic <strong>for</strong>mulations applied<br />

to those elements.<br />

Besides the differences <strong>in</strong> the exist<strong>in</strong>g <strong>for</strong>mulations found <strong>in</strong> literature to simulate<br />

the delam<strong>in</strong>ation phenomenon, all of them agree <strong>in</strong> divid<strong>in</strong>g the mesh where the<br />

crack is developed. This procedure is computationally very expensive, as it requires<br />

contact <strong>for</strong>mulations to avoid the <strong>in</strong>terpenetration of one body <strong>in</strong>to the other. And,<br />

also, all of them require an special <strong>for</strong>mulation where the delam<strong>in</strong>ation will occur,<br />

with <strong>in</strong>terface elements [1], cohesive zones [2] or with co<strong>in</strong>cident nodes, not connected<br />

to allow the mesh open<strong>in</strong>g, as it is done with the VCCT [8]. In contrast to<br />

the scope used by these authors to solve the delam<strong>in</strong>ation problem, this work uses<br />

the cont<strong>in</strong>uum mechanics to simulate the delam<strong>in</strong>ation <strong>in</strong>itiation and propagation,<br />

without mak<strong>in</strong>g any dist<strong>in</strong>ction of the elements <strong>in</strong> which delam<strong>in</strong>ation takes place.<br />

In this work, the Serial/Parallel (S/P) mix<strong>in</strong>g theory developed by Rastell<strong>in</strong>i [13],<br />

is used to obta<strong>in</strong> the composite per<strong>for</strong>mance and to simulate the delam<strong>in</strong>ation process.<br />

This theory is based on the def<strong>in</strong>ition of some compatibility equations between<br />

the stra<strong>in</strong>–stress states of the composite constituent materials. In the case of a composite<br />

made of fibre and matrix, what the Serial/Parallel mix<strong>in</strong>g theory does is to<br />

impose an iso–stra<strong>in</strong> condition on the parallel direction, usually the fibre direction,<br />

and a iso–stress condition on the serial direction, usually the rema<strong>in</strong><strong>in</strong>g directions<br />

of the stress and stra<strong>in</strong> tensors. With this scope, if the matrix structural capacity is<br />

lost, the S/P mix<strong>in</strong>g theory will reduce the structural capacity of fibre material <strong>in</strong><br />

the serial directions due to the iso–stress condition. Thus, it will be impossible <strong>for</strong><br />

the composite layer to develop shear or transversal stresses, less to transmit them to<br />

the surround<strong>in</strong>gs elements. The structural per<strong>for</strong>mance of a material <strong>in</strong> which serial

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