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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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Table 1: Material properties (Malandrino et al, 2011)<br />

Material E (MPa)<br />

Poisson’s<br />

ratio<br />

Initial<br />

Void Ratio<br />

Permeability<br />

(mm 4 /Ns)<br />

Annulus fibrosus 0.756 0.35 3.08 0.0002*<br />

Nucleus pulposus 0.388 0.17 4.88 0.0009*<br />

Cartilage endplate 20 0.4 4 0.0025*<br />

Bony endplate<br />

*From Eq. 1<br />

10,000 0.17 0.05 26,800<br />

a) b)<br />

c) d)<br />

Posterior IVD | Anterior IVD <br />

Fig. 1: Paths studied (red lines) represented on model 3 mesh: a) Path 1, b) Path 2, c)<br />

Path 3, d) Path 4.<br />

Green: AF; Blue: NP; Cream: Bony endplates; Purple: Cartilage endplate<br />

4. RESULTS<br />

Under extension, models 2, 3, and 4 led to similar SED predictions, whereas in axial<br />

rotation, neither model 2 nor model 3 converged to the results given by model 4 (Fig.<br />

2). For all models, FV oscillations occurred along the mid-sagittal plane (Fig. 3a).<br />

a) b)<br />

Fig. 2: SED predictions along Path 2, a) under extension and b) under axial rotation.<br />

Although SED calculations indicated that model 3 had not an optimal mesh size under<br />

axial rotation, this model was chosen to explore the FV instabilities because of the low<br />

computation time (1h) compared to model 4 (16h). Accordingly, oscillations were<br />

investigated only under sagittal extension.<br />

Among the strategies applied to avoid the oscillations, neither local refinement

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