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An Investigation on the use of Silicone to Model Arterial Tissue Behaviour in<br />

the Carotid Bifurcation<br />

Mulvihill, J.J., O'Donnell, M. R., O'Connell, B. M. and Walsh, M.T.<br />

Centre of Applied Biomedical Engineering Research, Dept. of Mechanical, Aeronautical and<br />

Biomedical Engineering and The Materials and Surface Science Institute, University of Limerick<br />

john.mulvihill@ul.ie<br />

Abstract<br />

This paper presents the investigation of an analogue<br />

material to represent arterial tissue behaviour. This<br />

study computationally compares the mechanical<br />

behaviour of arterial tissue and a silicone material<br />

model in an idealised carotid bifurcation model. Results<br />

demonstrate that silicone does not have similar<br />

mechanical behaviour as arterial tissue under a normal<br />

physiological pressure load.<br />

1. Introduction<br />

The development of atherosclerosis in the carotid<br />

bifurcation (CB) of the cardiovascular system has been<br />

the subject of much investigation. The CB is a prevalent<br />

area for atherosclerotic plaque build-up. Bhardvajet al.<br />

[1] dimensioned an idealised ‘Y’ shape model of the<br />

CB, which is the gold standard of dimensions for the<br />

CB in numerical studies (Haritonet al. [2]). However,<br />

Smith et al. [3] developed an updated CB idealised<br />

geometry that better represents the CB called the tuning<br />

fork model. A study by Thomas et al. [4] illustrated and<br />

validated the improvements in this model.<br />

Experimentally, silicone material is used primarily to<br />

mimic the mechanical behaviour of arterial tissue. This<br />

study aims to compare the mechanical behaviour of<br />

silicone material to arterial tissue using finite element<br />

analysis (FEA). These materials will be applied to the<br />

idealised CB tuning fork model.<br />

2. Material and Methods<br />

The numerical model was developed using FEA to<br />

model the mechanical behaviour of a silicone material<br />

and compare this material behaviour to the carotid<br />

arterial tissue. The silicone material was modelled using<br />

a reduced polynomial strain energy function (SEF)<br />

characterised and validated by Corbett et al. [5].The<br />

arterial tissue material model was applied using a SEF<br />

developed by Gasser et al., (HGO) [6]. This HGO SEF<br />

is a histological and phenomenological SEF that<br />

includes the effect of collagen fibres within the<br />

tissue.To determine if the HGO SEF does represent the<br />

mechanical behaviour of the carotid arterial tissue, and<br />

whether silicone behaves similarly, the numerical<br />

results are compared to the biaxial mechanical<br />

properties of common carotid arteries from Sommer et<br />

al., (2010) [7].<br />

3. Results<br />

The HGO SEF is compared to experimental data on<br />

the mechanical properties of carotid tissue from<br />

58<br />

Sommer et al. [7] as seen in figure 1. This was carried<br />

out to validate the HGO SEF and confirm that it<br />

predicts the arterial tissue behaviour.<br />

Figure 1 illustrates that the HGO SEF is comparable<br />

to experimental data under the same pressure loads.<br />

There is a difference in material behaviour after a 7%<br />

circumferential stretch. Figure 1 also compares the<br />

HGO SEF material behaviour to the silicone model<br />

showing a significant difference in mechanical<br />

behaviour between the material models.<br />

Figure 1:Plot of pressure against the circumferential stretch<br />

of the external radius for, the HGO SEF, Silicone SEF and the<br />

Sommer et al., (2010) [7] carotid artery properties<br />

4. Discussion<br />

The results from this study confirm that the HGO<br />

SEF is a good representation of arterial tissue to<br />

published experimental material properties, even when<br />

applied to a complex geometry such as the carotid<br />

bifurcation. The results from the numerical models<br />

illustrate the difference in mechanical behaviour<br />

between the silicone and arterial tissue. Silicone does<br />

not represent arterial tissue mechanical behaviour<br />

undergoing a pressure load. Therefore questions arise as<br />

to whether silicone is truly an analogous material of<br />

arterial tissue.<br />

5. References<br />

[1]Bhardvaj, B. K., Mabon, R. F. &Giddens, D. P. (1982).<br />

Journal of Biomechanics. 15: 363-365, 367-378.<br />

[2] Hariton, I., Debotton, G., Gasser, T. & Holzapfel, G.<br />

(2007). Bio.and Modelling in Mechanobiology. 6: 163-175.<br />

[3] Smith, R. F. (1996). Academic Radiology. 3: 898-911.<br />

[4] Thomas, J. B..(2005). Stroke. 36: 2450-2456.<br />

[5] Corbett, T. J. &McGloughlin, T. M. (2010). Journal of<br />

Biomechanical Engineering. 132: 011008-9.<br />

[6] Gasser, T. C., Ogden, R. W. & Holzapfel, G. A. (2006).<br />

Journal of The Royal Society Interface. 3: 15-35.<br />

[7] Sommer, G., Reitnig, P., Koltringer, L. & Holzapfel, G. A.<br />

(2010). Am J Physiol Heart Circ Physiol. 298: H898-912.

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