首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到18条相似文献,搜索用时 109 毫秒
1.
目的 利用数值模拟研究具有病人特异性的脑动脉瘤内的血液流动,为脑动脉瘤的破裂风险的评价和动脉瘤介入栓塞后复发风险的评价提供帮助。方法 从两例脑动脉瘤病人的3D-RA数据中重建动脉瘤几何模型,血液流变学模型选择假塑性非牛顿流体模型,利用商用CFD软件Fluent对两例动脉瘤内的血液流动进行数值模拟。结果 数值模拟给出了动脉瘤内的流线图、重要截面上的速度分布图、壁面上的切应力分布和压力分布图。并且绘制了在收缩期时刻动脉瘤颈部和瘤顶部各20个点上的壁面切应力和压力的变化情况。结论 血流动力学因素如流速、压力、壁面切应力、流动对壁面的冲击状况等因素与动脉瘤的生长和破裂密切相关,而由于脑动脉瘤形态各异、载瘤动脉与动脉瘤体的几何关系复杂,所以具有病人特异性的数值模拟对于研究动脉瘤破裂和复发风险具有重要价值。动脉瘤颈部的壁面切应力和壁面切应力的波动的变化规律并不相同,需要进一步研究壁面切应力的波动与脑动脉瘤生长与破裂之间的定量关系。  相似文献   

2.
目的分析在一个心动周期中蜿蜒型脑动脉瘤的血液流动情形、压力和壁面切应力分布和变化情况。方法构建了二维理想化的蜿蜒型脑动脉瘤(有2个动脉瘤)几何模型。利用计算流体力学方法对生理性脉动流进行了数值仿真。选择6个相继的心动时刻来显示流腔内的流动。结果2个流腔内的流动情形和壁面切应力分布呈现相似的特征,而第2个动脉瘤的末端瘤口则呈现非常高的壁面切应力和很高的压力梯度,这将更易于导致动脉瘤的发展和破裂。结论血液流动特征可以帮助人们更好地理解在S形弯曲动脉上滋生的在体蜿蜒型动脉瘤的血流动力学特性。  相似文献   

3.
目的 构建蜿蜒型动脉瘤和弯曲支架三维有限元模型,研究支架植入动脉瘤后的血流动力学的变化。方法 通过CAD软件构建出几何实体模型,借助有限元软件利用计算流体力学方法,分别对无支架和有支架的蜿蜒型脑动脉瘤定常流动血流动力学进行数值模拟,分析在动脉瘤中植入内支架前后的瘤腔内流动情形、压力和壁面切应力分布的变化情况。结果 有支架动脉瘤模型上游瘤腔内的血流速度被大大削弱,圆顶突起处局部高压力明显减弱,在下游瘤腔沿壁面的压力也得到明显降低并且分布也均衡了很多,末端唇缘处局部高切应力消失了,出现的是较小且均衡的切应力。结论 有支架模型瘤腔内的流速明显减小,均衡的压力分布与瘤腔内减弱的流动速度是相互统一的,利于瘤腔内血栓的形成。  相似文献   

4.
目的讨论非定常流动情况下,各参数对管壁压力和壁面切应力的影响,进而分析血液流动对内皮细胞和血管弹性的影响。方法应用两维对称模型模拟腹主动脉瘤中的非定常流动。结果Womersley数和Reynolds数越大,流动状态越复杂,涡的强度越大,对壁面切应力和压力都有很大的影响。结论壁面切应力和压力长期且快速的改变对内皮细胞和血管的强度产生影响,进而影响到动脉瘤的形成、成长和破裂。  相似文献   

5.
目的在考虑血管壁弹性条件下,分析颈内动脉血液流动和壁面切应力的分布特性,探讨动脉瘤破裂的生物力学因素。方法依据二维医学扫描图像构建三维个性化颈内动脉瘤模型。依据人体生理统计数据构建出血管壁模型。根据人体颈内动脉生理流动条件,利用有限体积法和有限元法模拟分析流固耦合作用下颈内动脉瘤中的血流动力学。结果在动脉瘤腔中有一个明显的涡旋存在,此涡旋流动的方向在心动周期内没有改变;在动脉瘤颈和动脉瘤壁面处存在一个壁面切应力值相对较大区域;在动脉瘤颈和动脉瘤顶有两个区域的Von Mises应力处于局部最大值。从材料强度角度考虑,这几个区域都是动脉瘤容易破裂的地方。结论通过流固耦合计算可以获得血管壁面应力分布特性,进而推断动脉瘤破裂的可能位置。  相似文献   

6.
区别于传统圆形截面丝支架,本研究中提出新型的三角形截面丝支架。与相同孔隙率的传统支架进行对比研究,探讨新型支架治疗颅内动脉瘤的血流动力学有效性。分别建立植入圆形截面丝支架、三角形截面丝支架和不植入支架动脉瘤三维有限元模型;设置相同的边界条件,利用流固耦合数值模拟的方法对流动阻力、速度、压力、壁面切应力和网格变形等参数进行了计算和分析。研究发现,三角形截面支架的流动阻力值小于圆形截面支架,并且植入三角形截面支架后动脉瘤的速度、压力、网格变形等参数在数值上均大于植入圆形截面支架模型,壁面切应力的峰谷值也有所增加。三角形截面支架针对梭形动脉瘤的治疗效果并不如圆形截面支架。在临床应用时,应考虑各项因素,择优而定。真正的临床应用效果,还需要进一步的实验验证。  相似文献   

7.
二维弹性动脉瘤模型的血液动力学数值模拟与分析   总被引:1,自引:0,他引:1  
本研究的目的在于探讨血液动力学参数对于动脉瘤形成、生长以及破裂的影响。从医学影像学图像出发,进行二维弹性动脉瘤模型的血液动力学数值模拟。将其结果与刚性动脉瘤结果在速度矢量场和切应力分布上进行对比,发现两者存在较大差异。主要表现在几个截面的速度分布有较大差异,其中一个出口的速度分布明显偏心,这将影响壁面的应力分布以及管壁物质交换。弹性和刚性模拟沿瘤壁的壁面切应力分布曲线走势基本相似,所不同的是两者的切应力数值特别是在瘤颈附近存在较大差异。通过分析阐明弹性壁模型更加符合临床与病理生理实际。研究结果对于分析动脉瘤形成、生长破裂以及预后有重要的临床应用价值。  相似文献   

8.
支架治疗主动脉弓内侧动脉瘤的仿真研究   总被引:15,自引:0,他引:15  
血管内支架是治疗主动脉弓动脉瘤的一种新技术。目前还没有人对具有局部突起的动脉瘤支架治疗血流动力学进行过研究。基于这样的事实,本仿真研究对主动脉弓内侧动脉瘤的支架治疗进行血流动力学分析。为便于比较,分别建立了有支架和无支架的主动脉弓动脉瘤模型。利用计算流体力学的方法对两个模型中的生理性血液流动进行了仿真。对流动情形、压力和壁面切应力分布进行了比较和分析,以便评价血管内支架对主动脉弓动脉瘤治疗的效果。结果表明,有支架的模型和无支架的模型,在瘤腔内的流动情形具有显著的不同。有支架模型瘤腔内的流动受到明显的抑制,特别是局部突起处的压力和壁面切应力大大地减小了。这些现象使我们有理由推断,血管内支架可以促进瘤腔内血栓的形成,并能减小动脉瘤破裂的危险。  相似文献   

9.
目的提出不同于传统支架的三角形网丝截面支架,并对其进行数值模拟,比较圆形、矩形、三角形截面支架在动脉瘤内的血流动力学效果。方法构建3个有支架植入的动脉瘤模型,分别为圆形(CM型)、矩形(RM型)和三角形(TM型)截面支架模型,并与1个无支架的动脉瘤模型(UM型)对照。在相同的边界条件下,利用有限单元法对4个模型进行流固耦合数值模拟。结果 RM型比TM型和CM型的速度更低、流阻更高、流转时间更长,所以矩形、三角形、圆形截面支架血液流动的影响效果依次降低。在削弱壁面切应力大小、降低壁面切应力波动性方面,RM型比TM型和CM型更加显著,但CM型和TM型的壁面升压低于RM型。壁面应力分布和变形结果表明动脉瘤沿远侧壁生长的可能性大于近侧壁,瘤顶破裂的风险最大。结论 3种截面支架展示了不同的血流动力学,这些结果为血管内支架的结构设计和优化提供了有意义的参考依据。  相似文献   

10.
半圆形截面支架介入串联囊状动脉瘤的血流动力学仿真   总被引:1,自引:0,他引:1  
为了研究半圆形截面支架对颅内串联囊状动脉瘤血流动力学的影响,针对同一动脉瘤结构,构建无支架和4种截面支架介入动脉瘤的有限元模型,分别命名无支架为U型、圆形截面为C型、半圆形截面圆面朝向瘤腔为ES型、圆面朝向血管轴向为IS型,然后对模型中的生理脉动流进行计算流体动力学仿真。数值模拟的结果显示:有支架模型的腔内流速被有效削弱,壁面附近的流速很低;血流对瘤腔的冲击减弱,壁面切应力的量值和波动性降低,分布均衡;腔内压力在支架介入后略有升高。对比分析两个瘤腔,流动情况和壁面切应力基本相同,下游瘤腔的压力低于上游瘤腔。IS型的仿真结果更好,这为支架的结构设计提供了一些理论指导。  相似文献   

11.
腹主动脉血管瘤的定常流动的模拟   总被引:1,自引:1,他引:0  
目的 应用两维对称模型模拟腹主动肪血管瘤的定常流动。方法 运用计算力学软件(FLUENTv4.3.2)进行数值模拟。结果 该研究给出了各种情况下的流动状态、流线分布、壁面剪切力和壁面压降的分布。结论 结果表明,腹主动脉血管瘤的形状和大小对流动状态影响不大,而雷诺数的增大会增大腹主动脉血管瘤内涡的强度。  相似文献   

12.
目的分别采用纯流体模型和流固耦合模型来计算腹主动脉瘤的血流动力学特征,比较两种数值模型的不同,并讨论在研究腹主动脉瘤中的应用。方法使用Gambit 2.2.30和COMSOL Multiphysics 4.2建立腹主动脉瘤的理想模型,分别基于有限体的方法分析纯流体模型,基于任意拉格朗日-欧拉算法(Arbitrary Lagrangian-Eulerian)计算流固耦合模型。结果同样的入口速度下,纯流体模型出现4个涡流和6个局部压力集中;流固耦合模型只有2个涡流和局部压力集中,且涡流中心更接近腹主动脉瘤的远端。在边界层分离点、血流回帖位置以及腹主动脉瘤的近端和远端,两种模型均出现壁剪切力极值。血管壁的最大形变和最大壁应力出现在腹主动脉瘤的近端和远端。结论两种模型的涡流个数和涡流中心的位置均不一样,与瘤体的生长有着密切的关联;流固耦合模型中的最大壁剪切力比纯流体模型要小36%;最大壁应力和最大血管壁的形变量与出口血压呈正相关。在研究血管瘤生长与血流动力学的关系时需要考虑使用流固耦合模型。  相似文献   

13.
As part of a general investigation on the effects of blood flow patterns in sidewall aneurysm, in vitro steady flow studies on rigid aneurysm models have been conducted using Particle Image Velocimetry over a range of Reynolds number from 200 to 1600. Above Reynolds number 700, one large recirculating vortex would be formed, occupying the entire aneurysmal pouch. The centre of the vortex is located at region near to the distal neck. A pair of counter rotating vortices would however be formed at Reynolds numbers below 700. For all the aneurysm models considered, the vortex strength, in general, is stronger at higher Reynolds numbers but lower at larger aneurysm size. Maximum strength of the vortex is about 15% of the bulk mean velocity in the upstream parent tube. Estimates of the wall shear stresses are derived from the near wall velocity measurements. Highest level of wall shear stresses always appears at the distal neck of the aneurysmal pouch. Stents and springs of different porosity have been used to dampen the flow movement inside the aneurysm so as to induce the possible formation of thrombosis. It is found that the flow movement inside the aneurysmal pouch can be suppressed to less than 5% of the bulk mean velocity by both devices. Furthermore, regions of high wall shear stresses at the distal neck could also be suppressed by almost 90%. The present results would be useful for further improvements in stent (or spring) technology.  相似文献   

14.
CFD modeling of blood flow following coil embolization of aneurysms   总被引:3,自引:0,他引:3  
In case of coil embolization of a giant or a multilobular aneurysm, it is difficult to fill an aneurysm sac completely with coils, therefore, partial blocking of an aneurysm sac is inevitable. Blood flow characteristics, which may influence embolization process of an aneurysm, are affected by the locations of coils for partially blocked aneurysms. Blood flow fields inside an aneurysm are also influenced by the geometry of a parent vessel. In order to suggest the coil locations effective for aneurysm embolization, the blood flow fields of lateral aneurysm models were analyzed for different coil locations and parent vessel geometries. Flow rate into an aneurysm sac from a parent vessel (inflow rate) and wall shear stress were also calculated. Inflow rates were smaller and low wall shear regions were larger in the distal neck blocked model comparing to the dome blocked models. In the distal neck blocked model, inflow volume was smaller by 31% (straight parent vessel model) and 34% (curved parent vessel model) comparing to other models. The time averaged values of normalized low wall shear regions were 4% and 12% greater in the distal neck blocked models with a straight and a curved parent vessel, respectively. Since smaller inflow and low wall shear stress provide hemodynamic environment promoting thrombus embolization, distal neck should be the effective coil location for aneurysm embolization.  相似文献   

15.
腹主动脉瘤几何形态对血液动力学影响的三维数值分析   总被引:2,自引:0,他引:2  
目的研究腹主动脉瘤不同形态学对瘤内血液动力学的影响,为临床预估动脉瘤的破裂提供参考。方法根据动脉瘤影像学上的特点建立不同几何形态的数学模型,采用计算流体动力学(CFD)方法,在周期性脉动速度入流、刚性壁面以及血液为牛顿流体的条件下,对一个心动周期内瘤内流场进行数值分析研究,比较不同几何形态腹主动脉瘤内血液动力学。结果非轴对称模型可造成相对较大的壁面剪应力;带有峰值偏移和曲率半径偏转的腹主动脉瘤,瘤内漩涡的发展变化会随着几何形态的不同而产生变化。结论腹主动脉瘤内流场特征的变化受到不同形态学的影响。  相似文献   

16.
Steady and pulsatile flow characteristics in rigid abdominal aortic aneurysm (AAA) models were investigated computationally (using Fluent v. 4.3) over a range of Reynolds number (from 200 to 1600) and Womersley number (from 17 to 22). Some comparisons with measurements obtained by particle image velocimetry under the pulsatile flow conditions are also included. A sinusoidal inlet flow waveform 1 + sin omega t with thin inlet boundary layers was used to produce the required pulsatile flow conditions. The bulk features of the mean flow as well as some detailed features, such as wall shear stress distributions, are the foci of the present investigation. Recirculating vortices appeared at different phases of a flow cycle causing significant spatial and temporal variations in wall shear stresses and static pressure distributions. A high level of shear stresses usually appeared at the upstream and downstream ends of the bulge. Effects of pressure rise caused by the increase in cross-sectional area were transmitted into the downstream tube. Further simulation studies were conducted using simulated physiological waveforms under resting and exercise conditions so as to determine the possible implication of vortex dynamics inside the AAA model.  相似文献   

17.
Steady and pulsatile flow characteristics in rigid abdominal aortic aneurysm (AAA)models were investigated computationally (using Fluent v.4.3) over a range of Reynolds number (from 200 to 1600)and Womersley number (from 17 to 22). Some comparisons with measurements obtained by particle image velocimetry under the pulsatile flow conditions are also included. A sinusoidal inlet flow waveform 1+sin omega t with thin inlet boundary layers was used to produce the required pulsatile flow conditions. The bulk features of the mean flow as well as some detailed features, such as wall shear stress distributions, are the foci of the present investigation. Recirculating vortices appeared at different phases of a flow cycle causing significant spatial and temporal variations in wall shear stresses and static pressure distributions. A high level of shear stresses usually appeared at the upstream and downstream ends of the bulge. Effects of pressure rise caused by the increase in crosssectional area were transmitted into the downstream tube. Further simulation studies were conducted using simulated physiological waveforms under resting and exercise conditions so as to determine the possible implication of vortex dynamics inside the AAA model.  相似文献   

18.
An endovascular technique using a stent has been developed and successfully applied in the treatment of wide neck aneurysms. A stent can facilitate thrombosis in the aneurysm pouch while maintaining biocompatible passage of the parent artery. Insertion of the stent changes the flow characteristics inside the aneurysm pouch, which can affect the intra-aneurysmal embolization process. The purpose of this study is to clarify the velocity and wall shear stress changes that are caused by stenting in fusiform and lateral aneurysm models. We used a flow visualization technique that incorporated a photochromic dye in order to observe the flow fields and measure the wall shear rates. The intra-aneurysmal flow motion was significantly reduced in the stented aneurysm models. Coherent inflow along the distal wall of the aneurysm was diminished and inflow was distributed along the pores of the stent wall in the stented models. Also, sluggish intra-aneurysmal vortex motion was well maintained in the stented aneurysm models during the deceleration phase. A less porous stent generally reduced the intraneurysmal fluid motion further, but the porosity effect was not significant. The magnitude and pulsatility of the wall shear rate were reduced by stenting, and the reductions were more significant in the lateral aneurysm models compared to the fusiform aneurysm models. The hemodynamic changes that were observed in our study can help explain the efficacy of in vivo thrombus formation caused by stenting. © 2002 Biomedical Engineering Society. PAC2002: 8719Uv, 8780-y, 8719Xx  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号