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Biomedical Engineering – From Theory to Applications

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456<br />

where<br />

<strong>Biomedical</strong> <strong>Engineering</strong> <strong>–</strong> <strong>From</strong> <strong>Theory</strong> <strong>to</strong> <strong>Applications</strong><br />

'<br />

Ik is the sum of the diagonal minors of k degree obtained by cutting the last three<br />

columns and rows in matrix [S].<br />

We can conclude that the eigenvalues depend on the values of the elastic constants, but the<br />

eigenvec<strong>to</strong>rs are, in part, independent of the values of the elastic constants<br />

5.3 The analytical expression for the staple compression force<br />

The stress vec<strong>to</strong>r can be written:<br />

Therefore, the specific deformation energy is:<br />

i Ei (20)<br />

i<br />

1 1<br />

U <br />

2 i i<br />

t<br />

i i<br />

(21)<br />

The orthopedic staple can be modeled as a bar which has an initial shape. When<br />

temperature increases the staple suffers deformations, changing its shape. Taking in<strong>to</strong><br />

account mechanical considerations, the deformation can be accepted as being caused by an<br />

exterior force which is applied <strong>to</strong> the free extremity. Thus, an increase of temperature, ΔT<br />

produces a displacement of the free extremity, Δw. The same displacement can be produced<br />

by a force (ΔP) which is applied in the free extremity. In fact, the force (ΔP) is a force <strong>to</strong> be<br />

applied in the free extremity. The <strong>to</strong>tal deformation energy is:<br />

1 1<br />

U dv<br />

2 i i<br />

D t<br />

i i (22)<br />

According <strong>to</strong> the Castigliano theorem energy, the derived strains of an elastic body<br />

compared with force value ΔP are similar <strong>to</strong> the displacement projection of the application<br />

point of the direction force (fig.1).<br />

U<br />

w <br />

Fig. 35. The loading schema for the Nitinol staple<br />

P<br />

In the case of small deformations we can accept that the stresses developed in the staple are<br />

proportional <strong>to</strong> the variation force ΔP. In these conditions, we can write:<br />

(23)

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