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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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DISCUSSION<br />

3D reconstruction of stent geometry during balloon inflation allows characterisation of<br />

the local deformation of stent units around the proximal and distal circumference. In<br />

addition, measures used in previous studies employing 2D methods which provide a<br />

more global assessment of changes in stent geometry have also been computed for<br />

comparison. The results shown in figure 5a are in good agreement with the results<br />

obtained by Kiousis et. al. [8]. The dog-boning ratio demonstrates greater deformation<br />

at both the proximal and distal ends within the range 3 to 6 atmospheres. During<br />

inflation of the 4mm stent the proximal end deformed first at an applied pressure value<br />

of 3.75 atmospheres. Further increase in pressure to 4.5 atmospheres caused full<br />

expansion of the stent, as shown in figure 5b.<br />

For the two stents observed in the current study, it is clear that the local deformation of<br />

individual stent units does not always correspond directly with changes in stent<br />

diameter. It was not possible to assess all stent units due to the field of view and stent<br />

rotation relative to the camera during balloon inflation. Figure 6 shows the expansion<br />

of two proximal and one distal unit. Results from the 3 mm diameter stent (Fig.6a)<br />

indicate that as the pressure load increased to 3 atmospheres the angle of the unit in the<br />

distal part increased significantly. These results are in good agreement with the<br />

computed dog-boning effect (Fig. 5a). However, the two units in the proximal part of<br />

the stent expand more gradually. This occurs due to smaller separation of chosen units<br />

and does not agree with the dog-boning response (Fig. 5a). Results from the 4 mm<br />

diameter stent (Fig. 6b) indicate the angle of the units in the proximal part increased<br />

significantly as the pressure load increased to 3.75 atmospheres whilst the distal unit<br />

remained unexpanded. This is also depicted in Fig. 4. This behaviour agrees with the<br />

dog-boning results (Fig. 5b) for both ends of the stent.<br />

CONCLUSION<br />

The present study computed both local and global measures of proximal and distal stent<br />

deformation under applied pressure. It has been shown that local strut deformation does<br />

not always correlate with changes in stent diameter. This may have implications for the<br />

local strains generated during contact of the stent with the vessel wall. The methods<br />

have been employed at coronary stent length scales and hence are appropriate for<br />

extension to the study of stent-vessel wall interaction.<br />

LIMITATIONS<br />

The present study considers the free expansion of the stent and does not consider the<br />

interaction of the stent with the vessel wall.<br />

ACKNOWLEDGEMENTS<br />

The research leading to these results has received funding from the European Union<br />

Seventh Framework Programme (FP7/2007-2013) under grant agreement n° 238113<br />

(project MeDDiCA).<br />

REFERENCES<br />

1. European cardiovascular disease statistics (2008)<br />

2. Duraiswamy, N, Schoephoerster, R. T., Moreno, M. R. and Moore J.E, Stented<br />

Artery Flow Patterns and Their Effects on the Artery Wall, Annu Rev Fluid Mech,<br />

2007, 39: p 357- 382.

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