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NUI Galway – UL Alliance First Annual ENGINEERING AND - ARAN ...

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Microstructural Modelling of Fatigue Crack Nucleation in Stents<br />

Sweeney, C. 1 , McHugh, P.E. 1 , Leen, S.B. 1<br />

1 Department of Mechanical and Biomedical Engineering & NCBES, <strong>NUI</strong> <strong>Galway</strong><br />

email: (c.sweeney4@nuigalway.ie)<br />

Abstract<br />

A methodology for modelling realistic microstructures<br />

of metallic materials is presented. The approach is<br />

applied to cyclic loading of stainless steel stents with a<br />

view to capturing the role of grain size distribution in<br />

fatigue crack nucleation.<br />

1. Introduction<br />

The use of balloon expandable stents as part of the<br />

angioplasty procedure has revolutionised the treatment<br />

of heart disease. Although stent design is a relatively<br />

mature topic, numerous instances of stent fatigue<br />

fracture have been reported, e.g. [1]. This is particularly<br />

the case recently with the advent of drug eluting stents<br />

where tissue in-growth over stent struts is impeded,<br />

allowing deformed geometries and fractures to be more<br />

clearly revealed than before. Hence, there is a clear<br />

need to gain a deeper understanding of stent fatigue<br />

behaviour and to develop fatigue failure prediction<br />

methods to aid stent design refinements. Typical stent<br />

strut dimensions are comparable with microstructural<br />

geometry, such as grain size [2-3], as shown in Fig. 1.<br />

Crystal plasticity (CP) modelling is therefore necessary<br />

to capture the inhomogeneity effects introduced by<br />

microstructure on deformation and hence fatigue<br />

behaviour of stents. Such a model will allow prediction<br />

and identification of microstructural phenomena during<br />

fatigue, including grain size effects [4] and crack<br />

nucleation mechanisms [5]. Voronoi tessellation is the<br />

first key step in this process, to model random<br />

microstructure of polycrystals [6].<br />

Initial work focuses on a well-known stent material:<br />

316 L stainless steel. A finite element micromechanical<br />

model of a representative volume element of<br />

polycrystalline 316 L was developed and used to<br />

simulate uniaxial cyclic loading for both continuum<br />

plasticity and CP formulations.<br />

2. Materials and Methods<br />

A Voronoi tessellation and Delaunay triangulation<br />

methodology was implemented into a Python script to<br />

generate a microstructural model representing<br />

inhomogeneous polycrystalline geometry. Tessellations<br />

with grain size distribution statistically close to that of a<br />

real microstructure were accepted (example shown in<br />

Fig. 1). An Abaqus user-material subroutine [2],<br />

incorporating an isotropic CP formulation, was<br />

employed. The stabilised cyclic response of the<br />

micromechanical model for strain-controlled uniaxial<br />

cyclic loading was then compared to the experimental<br />

macroscopic response.<br />

50<br />

75 µm<br />

100 µm<br />

Figure 1. Microscopy image of 316L stent strut<br />

[7] (foreground) and simulated microstructure.<br />

3. Results<br />

Good correlation was achieved between grain size<br />

distributions of the real and generated microstructures.<br />

Microscopic stress concentrations were predicted<br />

throughout the micromechanical model. CP material<br />

model constants were identified which agreed with the<br />

macroscopic cyclic stress range.<br />

4. Discussion<br />

A microstructural modelling methodology has been<br />

developed for realistic grain size distributions, capable<br />

of capturing inhomogeneity effects. The CP material<br />

model was calibrated to match macroscopic stress<br />

ranges for different applied strain ranges. Differences in<br />

hysteresis loop shapes, however, suggest that the next<br />

step involve the incorporation of a non-linear kinematic<br />

hardening formulation, e.g. [8], in the CP model. Future<br />

developments also include the introduction of a fatigue<br />

indicator parameter, such as accumulated plastic slip<br />

[5], to predict crack initiation during high-cycle fatigue.<br />

5. Acknowledgements<br />

Research funded by an IRCSET scholarship under<br />

the EMBARK initiative.<br />

6. References<br />

[1] Shaikh, F. et al., 2008. Catheter. .Cardiovasc. Interv.,<br />

71(5), 614-618.<br />

[2] You, X. et al., 2006. Acta. Mater., 54(18), 4825-4840.<br />

[3] Marrey, R.V. et al., 2006. Biomaterials, 27(9), 1988-2000.<br />

[4] Zhang, M., Neu, R. & McDowell, D., 2009. Int. J.<br />

Fatigue, 31(8-9), 1397-1406.<br />

[5] Manonukul, A. & Dunne, F.P.E., 2004. Proc. R. Soc.<br />

London Ser. A, 460(2047), 1881 -1903.<br />

[6] Kovac, M. & Cizelj, L., 2005. Nucl. Eng. Design, 235(17-<br />

19), 1939-1950.<br />

[7] Savage, P. et al., 2004. Ann. Biomed. Eng., 32(2), 202-<br />

211.<br />

[8] Barbe, F. et al., 2001. Int. J. Plasticity, 17(4), 513-536.

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