27.12.2012 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

was modelled as linear elastic, where Young’s Modulus, E = 4.2MPa and Poisson’s<br />

ratio, v = 0.3. Uni-axial compression force was applied on the platen using the same<br />

data applied to the experimental testing (Figure 3). All degrees of freedom of the platen<br />

were restricted, except in the axis parallel to the direction of the force applied. It was<br />

assumed that the bone material supporting the bottom surface of the cartilage was<br />

significantly stiffer than the cartilage tissue and hence, all degrees of freedom of the<br />

nodes on the bottom surface were restricted. Interactions between the platen and the<br />

cartilage surface were modelled as hard normal contact with no penetration and<br />

frictionless tangential contact. For comparison, an axis-symmetric flat surface cylinder<br />

model with the same thickness and diameter was analysed using the same material<br />

properties, boundary conditions and loading conditions (Figure 3).<br />

Figure 3 Diagram of the flat surface finite element model set up. Force was applied on the platen and the<br />

bottom surface of the explant was restricted in all degrees of freedom (left) Force loading applied in<br />

model and experimental testing, a maximum force of 11.58N was applied with a ramp of 0.1s. Force was<br />

held constant at 11.58N for 0.4s and the explant was unloaded again to 0.1N over 0.1s (right)<br />

4. RESULTS<br />

For the explant specific curvature model, maximum surface displacement at contact<br />

between the platen and explant was predicted to be 0.185mm and the maximum<br />

principal stress was 0.236MPa. Results for the flat surface model were found to be<br />

0.047mm and 0.030MPa (Figure 4).<br />

Figure 4 Comparison of maximum principal stress and nodal displacement predicted at contact point<br />

between the platent and explant<br />

Deformation pattern predicted by the flat surface model displayed uniform transverse<br />

isotropy across the explants, as local deformation decreased linearly with depth from<br />

0.047mm to 0mm. Maximum principal stress experienced across the tissue ranged from<br />

-0.0012MPa to 0.003MPa. No significant shear stresses or shear patterns was observed.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!