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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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Therefore, in order to examine the effect of microstructure of bone on the microcrack<br />

growth trajectory in transverse direction, various models were created and the effects of<br />

the fracture toughness and strength of the cement line and crack length were evaluated.<br />

The models were first created, and a background mesh of 4-noded tetrahedron cells was<br />

generated. We used just the nodes of these elements for representing the meshless<br />

models (Fig. 1b), the problem domains and their boundaries, and then we discarded the<br />

elements. So that, the background mesh of cells was used for integration of the system<br />

matrices. A displacement loading was applied at the bottom edge of each model and an<br />

initial edged microcrack was introduced into the models with orientation perpendicular<br />

to the loading direction, as shown in figure 1b. Then EFG Cohesive Fracture Method in<br />

LS-DYNA was implemented for fracture analysis. In current study, the extension of the<br />

crack was assumed to be of mode I – It is a current limitation of the method formulation<br />

in LS-DYNA. The interfaces between sub-domains of the models were perfect bounded.<br />

4. RESULTS AND DISCUSSION<br />

The first analysis focused on the role of cement lines in crack propagation behavior of<br />

cortical bone. For this purpose two different mesh-less models – Model A (absence of<br />

cement line) and Model B (presence of cement line) – were developed. In this case, the<br />

initial crack length was 303.8 [µm]. The interstitial bone and osteon have cohesive<br />

properties in common with each other and the cohesive properties of cement line were<br />

assumed some one third of cortical bone’s cohesive properties. After modeling and<br />

analysis with EFG cohesive fracture method in Ls-Dyna, the following were observed:<br />

In model A, the microcrack entered the osteon directly. In contrast, the crack deflected<br />

into the cement line and continued to grow within the cement line in model B (Fig. 3).<br />

(a) (b)<br />

Fig. 3. Simulation results of (a) osteon penetration in absence of the cement line and (b) crack<br />

deflection in presence of the cement line.<br />

Consistent with these observations, the cement line’s weak interface tends to deviate or<br />

stop microcrack propagation and thereby increases bone toughness. These results are, of<br />

course, dependent on cohesive fracture properties of cement line. The deviation is due<br />

to low fracture toughness and strength of cement line with respect to the interstitial bone<br />

and osteon. Meanwhile, the micro-architecture of Haversian cortical bone with changing<br />

the distribution of stress, in its turn, influences the microcrack propagation trajectories.

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