Numerical investigations of the haemodynamic changes associated with stent malapposition in an idealised coronary artery

被引:25
|
作者
Poon, Eric K. W. [1 ]
Barlis, Peter [1 ,2 ]
Moore, Stephen [3 ]
Pan, Wei-Han [1 ]
Liu, Yun [1 ]
Ye, Yufei [1 ]
Xue, Yuan [1 ]
Zhu, Shuang J. [1 ]
Ooi, Andrew S. H. [1 ]
机构
[1] Univ Melbourne, Melbourne Sch Engn, Dept Mech Engn, Melbourne, Vic 3010, Australia
[2] Univ Melbourne, Melbourne Med Sch, North West Acad Ctr, Melbourne, Vic 3010, Australia
[3] Univ Melbourne, IBM Res Collaboratory Life Sci Melbourne, Victoria Life Sci Computat Initiat, Melbourne, Vic 3010, Australia
基金
澳大利亚研究理事会;
关键词
Stent malapposition; Coronary stents; Atherosclerosis; in silico; Wall shear stress; SIROLIMUS-ELUTING STENT; INTRAVASCULAR ULTRASOUND ANALYSIS; ELEVATION MYOCARDIAL-INFARCTION; COMPUTATIONAL FLUID-DYNAMICS; OPTICAL COHERENCE TOMOGRAPHY; BLOOD-FLOW-VELOCITY; BARE-METAL STENTS; SHEAR-STRESS; CIRCULAR-CYLINDER; IMPLANTATION;
D O I
10.1016/j.jbiomech.2014.07.030
中图分类号
Q6 [生物物理学];
学科分类号
071011 ;
摘要
The deployment of a coronary stent near complex lesions can sometimes lead to incomplete stent apposition (ISA), an undesirable side effect of coronary stent implantation. Three-dimensional computational fluid dynamics (CFD) calculations are performed on simplified stent models (with either square or circular cross-section struts) inside an idealised coronary artery to analyse the effect of different levels of ISA to the change in haemodynamics inside the artery. The clinical significance of ISA is reported using haemodynamic metrics like wall shear stress (WSS) and wall shear stress gradient (WSSG). A coronary stent with square cross-sectional strut shows different levels of reverse flow for malapposition distance (MD) between 0 mm and 0.12 mm. Chaotic blood flow is usually observed at late diastole and early systole for MD=0 mm and 0.12 mm but are suppressed for MD=0.06 mm. The struts with circular cross section delay the flow chaotic process as compared to square cross-sectional struts at the same MD and also reduce the level of fluctuations found in the flow field. However, further increase in MD can lead to chaotic flow not only at late diastole and early systole, but it also leads to chaotic flow at the end of systole. In all cases, WSS increases above the threshold value (0.5 Pa) as MD increases due to the diminishing reverse flow near the artery wall. Increasing MD also results in an elevated WSSG as flow becomes more chaotic, except for square struts at MD= 0.06 mm. (C) 2014 Elsevier Ltd. All rights reserved.
引用
收藏
页码:2843 / 2851
页数:9
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