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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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curve for each sensor which varied over time corresponding to the loading and<br />

unloading of the femoral component. A custom program was developed in LabView<br />

that extracted the amplitude of each sensor’s displacement curve at 1 cycle intervals<br />

over the whole 40 cycles, this gave the values of inducible displacement due to loading<br />

for each sensor over the test period.<br />

Coordinate transformation theory for small angles [8] was then applied to allow the<br />

displacements (u, v, w) and rotations (θx, θy, θz) of the femoral component relative to<br />

the bone (or micromotions) to be determined for a fixed reference point (Fig. 1). If Uc,<br />

Vc and Wc are the displacements measured by DVRT 2, DVRT 1 and DVRT 3<br />

respectively; Va and Wa are the displacements measured by DVRT 6 and DVRT 5<br />

respectively; and Wb is the displacement measured by DVRT 4 then it can be shown that<br />

⎛U<br />

⎜<br />

⎜Va<br />

⎜<br />

⎝W<br />

a<br />

a<br />

U<br />

V<br />

b<br />

W<br />

b<br />

b<br />

Sensor input<br />

matrix<br />

The terms Ax, Ay, By, Cx, Cy represent the distance each target sphere is offset from the<br />

reference point as shown in Fig. 1c. Equation 1 can be simplified to give the required<br />

translational micromotions (u, v, w) and rotational micromotions (θx, θy, θz).<br />

4. RESULT<br />

Uc<br />

⎞ ⎛1<br />

⎟ ⎜<br />

Vc<br />

⎟ = ⎜θz<br />

W ⎟ ⎜<br />

c ⎠ ⎝−θ<br />

y<br />

−θ<br />

1<br />

θ<br />

x<br />

z<br />

θy<br />

⎞ ⎛ Ax<br />

⎟ ⎜<br />

−θx<br />

⎟×<br />

⎜ Ay<br />

1<br />

⎟ ⎜<br />

⎠ ⎝0<br />

Rotational matrix Offset matrix<br />

(Fig. 1c)<br />

0<br />

B<br />

0<br />

y<br />

Cx<br />

⎞ ⎛u<br />

⎟ ⎜<br />

Cy<br />

⎟ + ⎜v<br />

⎟ ⎜<br />

0 ⎠ ⎝w<br />

u ⎞ ⎛ Ax<br />

⎟ ⎜<br />

v ⎟ −⎜<br />

Ay<br />

w⎟<br />

⎜<br />

⎠ ⎝0<br />

Mean translational and rotational micromotions for the cases considered are shown in<br />

Fig. 2. It can be observed that all translational micromotions generally increase with<br />

flexion angle. If we examine the individual components of motion we can see that the<br />

largest translational micromotions occurred in the z direction (distal/proximal). For the<br />

flexion angles tested the z direction component of loading was the largest. Figure 2b<br />

shows that the addition of a short stem for both cemented and uncemented cases leads to<br />

a reduction in micromotions in comparison to implants with no stem (PS). The TS<br />

implant with long stem (Fig. 2c) shows significantly reduced micromotions in<br />

comparison to the other two implants. The translational micromotions reduce with<br />

cementing as expected in almost all cases. The trends with respect to rotations are<br />

considerably more complex. In general the largest rotations are found to occur with the<br />

uncemented PS implant. For long stem cases the rotational micromotions can be seen to<br />

be extremely small in comparison to the other two implants. Cementing is found to<br />

reduce rotational micromotions. The component of rotational micromotion found to be<br />

the smallest in general was θz (i.e rotation in the transverse plane).<br />

u<br />

v<br />

w<br />

Transformation<br />

matrix<br />

0<br />

B<br />

0<br />

y<br />

Cx<br />

⎞<br />

⎟<br />

Cy<br />

⎟<br />

⎟<br />

0 ⎠<br />

Offset matrix<br />

(Fig. 1c)<br />

(1)

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