NUI Galway – UL Alliance First Annual ENGINEERING AND - ARAN ...
NUI Galway – UL Alliance First Annual ENGINEERING AND - ARAN ...
NUI Galway – UL Alliance First Annual ENGINEERING AND - ARAN ...
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Development of a mixed-mode cohesive zone model for stent and cell<br />
applications<br />
Ó Máirtίn, É. 1,2 1, 2<br />
, McGarry, P.<br />
Department of Mechanical and Biomedical Engineering, National University of Ireland, <strong>Galway</strong>,<br />
e.omairtin1@nuigalway.ie<br />
Abstract<br />
Cohesive zone models have been commonly used to<br />
simulate coating delamination from a substrate and<br />
crack propagation in certain material types [1]. In this<br />
study we develop a path-dependent cohesive zone<br />
model (CZM). The CZM is then applied to two distinct<br />
case studies: (i) mixed-mode cell debonding during<br />
cyclic substrate stretching and (ii) mixed-mode<br />
overclosure of a stent coating during stent deployment.<br />
Unphysical mixed-mode behaviour is computed for<br />
cohesive zone model formulations derived from an<br />
interface potential function.<br />
1. Introduction<br />
In this study we present a potential-based, coupled<br />
cohesive zone formulation which has been used to<br />
describe many mixed-mode delamination processes. We<br />
propose an alternative, path-dependent cohesive zone<br />
model in an effort to simulate physically realistic mixedmode<br />
behaviour at an interface.<br />
2. Materials and Methods<br />
A path-dependent CZM is developed whereby<br />
interface tractions, Ti, are related to interface<br />
separations, Ui, by<br />
2<br />
U <br />
Ti AiU<br />
i exp 1 exp U<br />
where i= 1,2. Subscripts 1 and 2 refer to normal and<br />
tangential directions respectively. The constants Ai<br />
define the independent interface strengths in the 1 and 2<br />
directions.<br />
Simulations are also performed using a potentialbased<br />
cohesive zone model whereby tractions are<br />
derived from an interface potential function [2],<br />
ø(U1,U2):<br />
i<br />
This requires the definition of n and t; the work of<br />
normal and tangential interface separation, respectively.<br />
Cohesive zone formulations are implemented by means<br />
of UINTER user-defined subroutine in Abaqus ©<br />
Ti U1<br />
U 2 U<br />
software.<br />
, <br />
3. Results<br />
Repulsive normal tractions develop during mixedmode<br />
cell separation following application of potentialbased<br />
model. The cell is forced away from the substrate<br />
at 0% substrate strain, preventing the formation of new<br />
bonds (Figure1(a)).<br />
2<br />
69<br />
Repulsive normal<br />
forces<br />
(a)<br />
Application of the path-dependent model produces a<br />
more realistic result where bond formation occurs at the<br />
end of each strain cycle (Figure1(b)).<br />
(a)<br />
1<br />
0.5<br />
0<br />
-0.5<br />
0 1 2 3 4 5<br />
Time (seconds)<br />
Figure 1. Normal traction and separation results<br />
following application of (a) potential-based CZM and<br />
(b) path-dependent CZM at the cell-substrate interface<br />
(b)<br />
Application of the potential-based model produces<br />
unrealistic coating overclosure and no coating buckling<br />
occurs (Figure2(a)). Overclosure is prevented when<br />
path-dependent model is used with significant buckling.<br />
4. Discussion<br />
Unrealistic repulsive tractions are computed for<br />
mixed-mode cell separation when a potential-based<br />
cohesive zone model is applied at a cell-substrate<br />
interface.<br />
Unrealistic mixed-mode coating overclosure is<br />
computed when a potential-based model is applied at a<br />
stent-coating interface. Implementation of a pathdependent<br />
model leads to more physically realistic<br />
mixed-mode behaviour.<br />
8. References<br />
[1] Y. Yan, F. Shang, “Cohesive zone modeling of interfacial<br />
delamination in PZT thin films”, Int.J.Solids Struct,<br />
Publisher, Location, 2009, 46(13), pp. 2739-2749.<br />
[2] X. P.. Xu, A. Needleman, “Void nucleation by inclusion<br />
debonding in a crystal matrix”, Modell. Simul. Mater. Sci.<br />
Eng, 1994, 1(2), pp.111-132.<br />
(b)<br />
-1<br />
0 1 2 3 4 5<br />
Time (seconds)<br />
Figure 2. Coating deformation after application of<br />
(a) potential-based model and (b) path dependent<br />
model at the stent-coating interface<br />
1<br />
0.5<br />
0<br />
-0.5