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Computational Methods for Debonding in Composites

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6 Study of Delam<strong>in</strong>ation with <strong>in</strong> <strong>Composites</strong> 121<br />

stresses are zero is similar, as it will be proved <strong>in</strong> this work, to the per<strong>for</strong>mance<br />

shown by a delam<strong>in</strong>ated material.<br />

To obta<strong>in</strong> this structural behaviour, the matrix material has to loose its strength <strong>for</strong><br />

a certa<strong>in</strong> stress state. This lost of strength must be permanent <strong>in</strong> order to simulate the<br />

real crack produced by delam<strong>in</strong>ation <strong>in</strong> the material. This is achieved with a damage<br />

<strong>for</strong>mulation based on the fracture energy of the material.<br />

A detailed description of the different <strong>for</strong>mulations required to simulate the<br />

delam<strong>in</strong>ation process: the S/P mix<strong>in</strong>g theory and the damage <strong>for</strong>mulation used <strong>in</strong><br />

matrix material, are described <strong>in</strong> the follow<strong>in</strong>g section. Afterwards, to prove the<br />

validity of the scope used to simulate the delam<strong>in</strong>ation phenomenon, as well as the<br />

ability of the <strong>for</strong>mulations proposed to simulate it, this work compares the results<br />

obta<strong>in</strong>ed from the experimental test made to obta<strong>in</strong> the mode II fracture energy of a<br />

composite with the results obta<strong>in</strong>ed from a numerical simulation of the same model.<br />

The experimental test is the End Notch Flexure (ENF) test def<strong>in</strong>ed by the European<br />

Structural Integrity Society (ESIS). The agreement between experimental and<br />

numerical results will prove the ability of the S/P mix<strong>in</strong>g theory, together with the<br />

damage <strong>for</strong>mulation used, to simulate delam<strong>in</strong>ation processes.<br />

6.2 Formulation<br />

The <strong>for</strong>mulation shown <strong>in</strong> this work to simulate the delam<strong>in</strong>ation effect <strong>in</strong> composite<br />

materials made of lam<strong>in</strong>ates of fibre re<strong>in</strong><strong>for</strong>ced polymers is the follow<strong>in</strong>g<br />

one: The composite behaviour is obta<strong>in</strong>ed from its constituent materials with the<br />

serial/parallel mix<strong>in</strong>g theory developed by Rastell<strong>in</strong>i [13]. This theory is described<br />

<strong>in</strong> Sect. 6.2.1. To obta<strong>in</strong> a good convergence ratio <strong>in</strong> the process and, <strong>in</strong> most cases,<br />

to be able to obta<strong>in</strong> convergence, it is necessary to use a tangent constitutive tensor.<br />

This tensor can be obta<strong>in</strong>ed analytically <strong>for</strong> some constitutive equations but not<br />

<strong>for</strong> the damage <strong>for</strong>mulation used <strong>in</strong> the presented simulation. To solve this problem,<br />

the tangent constitutive tensor is obta<strong>in</strong>ed per<strong>for</strong>m<strong>in</strong>g a numerical derivation<br />

with a perturbation method. This methodology is exposed <strong>in</strong> Sect. 6.2.2. F<strong>in</strong>ally, the<br />

delam<strong>in</strong>ation process is obta<strong>in</strong>ed as a lost of strength and stiffness <strong>in</strong> matrix material.<br />

This effect is characterized us<strong>in</strong>g a damage <strong>for</strong>mulation, which is described <strong>in</strong><br />

Sect. 6.2.3.<br />

6.2.1 Serial/Parallel Mix<strong>in</strong>g Theory<br />

The serial/parallel mix<strong>in</strong>g theory considers that <strong>in</strong> a certa<strong>in</strong> direction (or directions)<br />

the compound<strong>in</strong>g materials behave <strong>in</strong> parallel, while their behaviour is serial <strong>in</strong> the<br />

rema<strong>in</strong><strong>in</strong>g directions. For this reason it is necessary to def<strong>in</strong>e, and split, the serial and<br />

parallel parts of the stra<strong>in</strong> and stress tensors. This is done with two complementary<br />

fourth order projector tensors, one correspond<strong>in</strong>g to the serial direction (PS)andthe

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