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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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5. DISCUSSION<br />

A musculoskeletal numerical model of the upper limb was developed. The anatomical data was<br />

taken from the Visible Human Project [15][16]. It includes the three joints participating in humerus<br />

movement. They are spanned over by 28 muscle fibres. Displacement boundary conditions on the<br />

humeral head are released during the movement, to allow its displacement. To solve the mechanical<br />

indetermination of the muscle force distribution, an optimization algorithm is used. Mean square<br />

muscle stresses are minimized. The model is used to simulate an abduction movement in the scapula<br />

plane. Muscle forces, reaction forces in the glenohumeral joint, humeral head translation and<br />

loading patterns on the glenoid cartilage are computed.<br />

The obtained muscle forces are in principle in agreement with results from the literature [5][20].<br />

The anterior parts of the deltoid are active during the entire motion making a bell curve with the<br />

maximum situated around 90◦ absolute abduction. Nevertheless, posterior parts of the deltoid rest<br />

almost inactive. This does not correspond with in-vivo measurements [14]. The loading of the glenohumeral<br />

joint is in agreement with the results found in literature [21]. In-vivo measurements<br />

showed a continuous rise to 60-70% BW from 0° to 90° abduction. Peak forces of 80-90% BW<br />

were measured at maximum abduction angles. Although the local minimum of the computed forces<br />

at 120° is not documented in experimental data, the general trend of rising joint loading during abduction<br />

is visible in the numerical results. The directions of humeral head translations are in agreement<br />

with experimental data [11] but too large in magnitude. Contact pressure on the cartilage correspond<br />

to experimental data [22]. The joint loadings of 440 N used in experiments correspond to<br />

an abduction angle of 70°. During the whole movement cartilage pressure is lower than injuries<br />

joint loadings [23].<br />

The model has still some limitations. Concerning the muscle modelling, it is known that maximal<br />

muscle forces are not only dependent on physiological cross sections, but also on actual length, contraction<br />

rates and contraction/relaxation mode [24]. First approaches in that direction show a significant<br />

change in muscle force distribution with a higher number of active muscles during the whole<br />

simulation. Furthermore, changes of muscle moment arms due to tissue deformation during movements<br />

can not be reproduced with 1D muscle modelling. The large humeral head translations can be<br />

traced back to the fact, that glenohumeral reaction forces are restricted by the direction criteria<br />

throughout the whole movement. In consequence, the humeral head moves along the cartilage border.<br />

This results in the maximum possible translation range. If the direction criteria is strengthened<br />

to less than 50% of the glenoid cartilage surface, humeral head translation can be forced to reproduce<br />

experimental results, but leads to significant higher joint loadings. As the humeral head translations<br />

are too large, the contact zones are distributed along the cartilage border.<br />

Although the humeral head translation seems excessive, the stabilization method of the humeral<br />

head is working. Displacement boundary conditions can be removed during the movement and humeral<br />

head translation can be simulated. Furthermore, glenohumeral joint loadings show promising<br />

results.<br />

We have shown that a direction criteria on reaction forces of the glenohumeral joint can govern the<br />

stability problem, but whether leads to large humeral head translations or large joint loadings. If optimization<br />

routines are used to compute muscle forces, monitoring of humeral head translation<br />

needs to be included into the optimization routine and the computation of rotator cuff muscle activities<br />

might be handled differently.<br />

6. REFERENCES<br />

1. N.K. Poppen and P.S. Walker: Forces at the glenohumeral joint in abduction, Clinical<br />

Orthopedics, 1<strong>978</strong>, 135, 165-170<br />

2. C. Högfors, G. Sigholm and P. Herberts: Biomechanical model of the human shoulder -<br />

I.Elements, Journal of Biomechanics, 1987, 20(2), 157-166

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