Ramiar Abas, Larimi Morsal Momenti, Ranjbar Ali Akbar
Faculty of Mechanical Engineering, Noshirvani University of Technology, Babol, Iran.
Acta Bioeng Biomech. 2017;19(3):27-41.
Hemodynamic factors, such as Wall Shear Stress (WSS), play a substantial role in arterial diseases. In the larger arteries, such as the carotid artery, interaction between the vessel wall and blood flow affects the distribution of hemodynamic factors. The fluid is considered to be non-Newtonian, whose flow is governed by the equation of a second-grade viscoelastic fluid and the effects of viscoelastic on blood flow in carotid artery is investigated.
Pulsatile flow studies were carried out in a 3D model of carotid artery. The governing equations were solved using finite volume C++ based on open source code, OpenFOAM. To describe blood flow, conservation of mass and momentum, a constitutive relation of simplified Phan-Thien-Tanner (sPTT), and appropriate relations were used to explain shear thinning behavior.
The first recirculation was observed at t = 0.2 s, in deceleration phase. In the acceleration phase from t = 0.3 s to t = 0.5 s, vortex and recirculation sizes in bulb regions in both ECA and ICA gradually increased. As is observed in the line graphs based on extracted data from ICA, at t = 0.2 s, τyy is the maximum amount of wall shear stress and τxy the minimum one. The maximum shear stress occurred in the inner side of the main branch (inner side of ICA and ECA) because the velocity of blood flow in the inner side of the bulb region was maximum due to the created recirculation zone in the opposite side in this area.
The rheology of blood flow and shear stress in various important parts (the area that are in higher rates of WSS such as bifurcation region and the regions after bulb areas in both branches, Line1-4 in Fig. 7) were also analyzed. The investigation of velocity stream line, velocity profile and shear stress in various sections of carotid artery showed that the maximum shear stress occurred in acceleration phase and in the bifurcation region between ECA and ICA which is due to velocity gradients and changes in thinning behavior of blood and increasing strain rate in Newtonian stress part.
血流动力学因素,如壁面剪应力(WSS),在动脉疾病中起着重要作用。在较大的动脉中,如颈动脉,血管壁与血流之间的相互作用会影响血流动力学因素的分布。流体被视为非牛顿流体,其流动由二级粘弹性流体方程控制,并研究了粘弹性对颈动脉血流的影响。
在颈动脉的三维模型中进行脉动流研究。基于开源代码OpenFOAM,使用有限体积C++求解控制方程。为了描述血流,使用了质量和动量守恒、简化的Phan-Thien-Tanner(sPTT)本构关系以及适当的关系来解释剪切变稀行为。
在减速阶段,t = 0.2 s时观察到第一次回流。在从t = 0.3 s到t = 0.5 s的加速阶段,颈外动脉(ECA)和颈内动脉(ICA)球部区域的涡旋和回流尺寸逐渐增大。从ICA提取的数据绘制的线图中可以看出,在t = 0.2 s时,τyy是壁面剪应力的最大值,τxy是最小值。最大剪应力出现在主分支内侧(ICA和ECA内侧),因为球部区域内侧的血流速度最大,这是由于该区域另一侧形成了回流区。
还分析了血流的流变学和剪切应力在各个重要部位(如分叉区域和两个分支球部区域之后的区域等高壁面剪应力区域,图7中的Line1-4)的情况。对颈动脉不同截面的速度流线、速度剖面和剪应力的研究表明,最大剪应力出现在加速阶段以及ECA和ICA之间的分叉区域,这是由于速度梯度、血液剪切变稀行为的变化以及牛顿应力部分应变率的增加所致。