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Computational Methods for Debonding in Composites

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7 Interaction Between Intraply and Interply Failure <strong>in</strong> Lam<strong>in</strong>ates 155<br />

For the evaluation of the traction, the equivalent displacement jump is calculated<br />

via<br />

�<br />

δb = 〈δn〉 2 + δ 2 r<br />

(7.62)<br />

where subscript b refers to the current mixed mode and δr is def<strong>in</strong>ed as the total shear<br />

displacement jump: δ 2 r = δ 2 s + δ 2<br />

t . Normal relative displacements only contribute<br />

when positive, hence the use of the MacAuley operator, which is def<strong>in</strong>ed as 〈x〉 =<br />

(x + |x|)/2.<br />

The mixed mode ratio β and the related variable B are computed accord<strong>in</strong>g to<br />

β =<br />

B =<br />

δr<br />

δr + 〈δn〉<br />

β 2<br />

1 + 2β 2 − 2β<br />

(7.63)<br />

(7.64)<br />

The onset criterion and the propagation criterion <strong>for</strong> the current mixed mode ratio<br />

are<br />

δ 0 b =<br />

�<br />

(δ 0 n ) 2 �<br />

+ (δ 0 r ) 2 − (δ 0 n ) 2�<br />

Bη (7.65)<br />

and<br />

δ f<br />

b =<br />

δ 0 n δ f<br />

�<br />

n + δ 0 r δ f<br />

r − δ 0 n δ f<br />

�<br />

n Bη δ 0 (7.66)<br />

b<br />

respectively, where η is a material parameter that is to be obta<strong>in</strong>ed from experimental<br />

data and is related to mode <strong>in</strong>teraction.<br />

With this, the bil<strong>in</strong>ear constitutive law <strong>for</strong> the current mixed mode ratio is complete<br />

and the damage variable can be updated. Upon monotonic load<strong>in</strong>g, the damage<br />

variable, d, is calculated with<br />

f �<br />

δb δb − δ<br />

d = 0 �<br />

� b<br />

δb δ f<br />

b − δ 0 � , d ∈ [0,1] (7.67)<br />

b<br />

To obta<strong>in</strong> the correct load<strong>in</strong>g-unload<strong>in</strong>g-reload<strong>in</strong>g behavior, the follow<strong>in</strong>g condition<br />

is added<br />

d˙ ≥ 0 (7.68)<br />

which demands storage of d as history variable at each <strong>in</strong>tegration po<strong>in</strong>t, similar to<br />

the description by Jiang et al. [12], which is different from the description by Turon<br />

et al. [25], where the maximum total displacement jump, δb, is stored as history<br />

variable and substituted <strong>in</strong>to Eq. (7.67).

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