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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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, <br />

, <br />

,<br />

<br />

, <br />

(3)<br />

where is the 5-order vector of coefficients: , , , , .<br />

This polynomial was defined as class <br />

, because the second derivatives is linked to<br />

each other for every subset i, as follows:<br />

,1 ,0 2 , <br />

,1 ,0 ,1 ,0 (4)<br />

Furthermore, we set:<br />

<br />

<br />

1, <br />

<br />

<br />

<br />

,0 ,1 (5)<br />

,0 <br />

,1 <br />

respecting the link relation:<br />

1, 1, ,1 ,0 0 (6)<br />

Whereas (3) denoted 5n coefficients, equations (4) and (5) led us to 5N-1 linear<br />

equations. As a consequence, a cubic spline 0 was used on the last interval . Then, considering that joint coordinates provided from the measurement, the<br />

coefficients appeared as a function of a vector to optimize which collects the joint<br />

accelerations:<br />

, , … , 0, … , , … , (7)<br />

The coefficients were deduced from the linear resolution of:<br />

Φ (8)<br />

Finally, over the interval [0,T], we wrote the following approximations:<br />

<br />

, <br />

, <br />

<br />

, <br />

which led to the rewriting criterion:<br />

(9)<br />

∑ , , , , , <br />

<br />

(10)<br />

Accounting that polynomial coefficients involve measured joint coordinates, the<br />

parametric optimization stayed unconstrained and timeless consuming consequently.<br />

3.2. Experimentation and inverse dynamics<br />

Our approach was tested using a flexion-entension movement performed at self-selected<br />

velocity on a force plate (Kistler, Switzerland) setting at 1000Hz. Kinematic data were<br />

recorded at 50Hz using a motion analysis system (Biogesta, France). The joint<br />

coordinates were provided from sixteen markers (top of head, spinous process of<br />

the 7 th cervical vertebrae, acromio-clavicular joint, lateral elbow epicondyle, radius<br />

styloid, great trochanter, lateral knee epicondyle, lateral maleous, second metatarsal<br />

head). Their positions were low-pass filtered at 6Hz with a zero-lag Butterworth fourorder<br />

filter. A finite centred differentiation was used to determine the first ( ) and

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