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ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

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4.2 Case NG09<br />

The numerical impact simulation predicts fracture patterns on the frontal bone as<br />

illustrated in Figure 3. The linear fracture through the left orbita is not predicted since<br />

the face has only a linear elastic behaviour in the model. Therefore, the fracture pattern<br />

stops on the frontier between the skull and the face. Nevertheless, a global fracture<br />

region is predicted by the model even if the location is not as accurate as the one<br />

observed in the experience. In terms of interaction force between the head and the<br />

impacting mass, the numerically calculated amplitude reaches the same level than the<br />

experimentally measured one as illustrated in Figure 3. Moreover, the duration of that<br />

first impact is the same in the experimental impact as in the numerical impact. Besides,<br />

the numerical simulation shows a second impact which is also observable in the<br />

experience with approximately the same amplitude and duration. Eventually, the<br />

calculated global strain energy of the skull reaches levels of 12,000 mJ and thus allows<br />

the model to predict skull fracture since the limit relies on 833 mJ.<br />

Figure 3: Skull deleted elements numerical prediction (left), and experimental (blue)<br />

and numerical (pink) interaction force between the head and the impactor (right).<br />

4.3 Case NG15<br />

The numerical impact simulation predicts fracture patterns on the frontal bone as<br />

illustrated in Figure 4. It can be concluded that the multiple fracture patterns extending<br />

to left temporal are basically predicted by the model. In terms of interaction force<br />

between the head and the impacting mass, the numerically calculated amplitude is 3,000<br />

N higher than the experimentally measured one as illustrated in Figure 4. Nevertheless,<br />

the first impact duration is the same in the experimental impact as in the numerical<br />

impact. Moreover, the numerical simulation shows a second impact which is also<br />

observable in the experience but with a lower amplitude. Eventually, the calculated<br />

global strain energy of the skull reaches levels of 22,000 mJ and thus allows the model<br />

to predict skull fracture since the limit relies on 833 mJ.<br />

Figure 4: Skull deleted elements numerical prediction (left), and experimental (blue)<br />

and numerical (pink) interaction force between the head and the impactor (right).

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