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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

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the difference in percentage between the compression force obtained in the simulation<br />

of breast compression considering gravity and without considering it.<br />

Table 5. Difference between the compression force obtained in the simulation of breast<br />

compression considering gravity and without considering it (%).<br />

Patient<br />

Differences for the<br />

linear elastic model<br />

Differences error for<br />

the Neo-Hookean<br />

model<br />

Differences for<br />

Mooney-Rivlin<br />

model<br />

Differences for the<br />

Polynomial model<br />

P1 8.72% 7.07% 0.44% 6.74%<br />

P2 9.48% 31.46% 0.15% 11.12%<br />

P3 8.39% 2.58% 0.44% 1.45%<br />

P4 27.09% 5.88% 6.16% 8.22%<br />

P5 36.21% 10.91% 5.25% 14.81%<br />

P6 21.26% 6.51% 0.02% 7.26%<br />

5. DISCUSSION<br />

The real compression force obtained ranged from 78 to 138 N. This agrees with<br />

Sullivan et al. in [15] where the values ranged from 49 to 186.2 N. In our case, none of<br />

the four models used in this work matched the real compression force for all patients.<br />

The linear elastic and Neo-Hookean models provided values under of this range.<br />

Mooney-Rivlin model was close to these values for two cases (P1, P4) where the real<br />

forces were (118 N, 108 N), respectively. However, for the other four patients, greater<br />

values were obtained for the compression forces which were far to be in the range. The<br />

values obtained for the polynomial model where within the range of the real forces in<br />

three cases (P1, P4, and P5), although, it was not possible to achieve the real forces<br />

which were (118N, 108N, 137N). However, the values obtained for the rest of patients<br />

were no so far of the real force range as in the case of considering the Mooney-Rivlin<br />

model. These results suggest that a Polynomial model could represent the behavior of<br />

the breast compression accurately, although the parameter should be measured for each<br />

patient specifically. On the other hand, prone gravity-loaded breast should not be used<br />

as an approximation of unloaded reference state for X-ray mammography simulation,<br />

since important errors can be committed (Table 5). Although low differences between<br />

the compression forces were obtained for the Mooney-Rivlin model, these models do<br />

not provide compression forces closer to the real ones.<br />

6. CONCLUSIONS<br />

This work has proved that prone gravity-loaded breast should not be used as an<br />

approximation of non-deformed state for X-ray mammography simulation since errors<br />

of about 10% could be committed. However, the approximation to the zero-strain state<br />

of the breast presented in this work, which take into account the gravity, can be used for<br />

more accurate simulations of the breast compression during an X-ray mammography.<br />

7. ACKNOWLEGMENTS<br />

This work has been partially funded by the Spanish Ministry of and Science and

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