Simulation of mechanical behavior of temperature-responsive braided stents made of shape memory polyurethanes

Abstract Polymeric stents can be considered as an alternative to metallic stents thanks to their lessened incidence of restenosis and controlled deployment. The purpose of this study was to investigate the feasibility of developing a temperature-responsive braided stent using shape memory polyuretha...

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Bibliographic Details
Published inJournal of biomechanics Vol. 43; no. 4; pp. 632 - 643
Main Authors Hyun Kim, Ju, Jin Kang, Tae, Yu, Woong-Ryeol
Format Journal Article
LanguageEnglish
Published Kidlington Elsevier Ltd 03.03.2010
Elsevier
Elsevier Limited
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Summary:Abstract Polymeric stents can be considered as an alternative to metallic stents thanks to their lessened incidence of restenosis and controlled deployment. The purpose of this study was to investigate the feasibility of developing a temperature-responsive braided stent using shape memory polyurethane (SMPU) through finite element analysis. It was assumed that braided stents were manufactured using SMPU fibers. The mechanical behavior of SMPU fibers was modeled using a constitutive equation describing their one-dimensional thermal-induced shape memory behavior. Then, the braided stents were analyzed to investigate their mechanical behavior using finite element analysis software, in which the constitutive equation was implemented through a user material subroutine. The diameter of the SMPU fibers and braiding angle were chosen as the design parameters and their values were adjusted to ensure that the mechanical properties of the braided polymer stents match those of metallic stents. Finally, the deployment process of the braided stents inside narrowed vessels was simulated, showing that the SMPU stents can be comfortably implanted while minimizing the overpressure onto the vessel walls, due to their thermo-responsive shape memory behavior.
Bibliography:ObjectType-Article-1
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content type line 23
ISSN:0021-9290
1873-2380
DOI:10.1016/j.jbiomech.2009.10.032