Giannakoulas George, Giannoglou George, Soulis Johannes, Farmakis Thomas, Papadopoulou Stella, Parcharidis George, Louridas George
1st Department of Cardiology, AHEPA University General Hospital, Stilp. Kiriakidi 1, Thessaloniki, Greece.
Med Hypotheses. 2005;65(6):1191-5. doi: 10.1016/j.mehy.2005.06.017. Epub 2005 Aug 16.
Computational cardiovascular mechanics has allowed scientists to create complex 3D models for the simulation of cardiovascular problems. Mechanical stress plays a crucial role in the function of the cardiovascular system; stress analysis is a useful tool for the understanding of vascular pathophysiology. By using the spiral CT imaging and computational structural analysis, we present a noninvasive method of wall stress analysis in the normal aorta. The aortic segment was extended from the origin of the inferior mesenteric artery to the aortic bifurcation. The length of this segment was 12 cm, while the maximum transverse diameter was 2.075+/-0.129 cm. A 3D aortic model was constructed based on the CT scan images. The aorta was assumed to have a uniform wall thickness of 1.5mm. The generated unstructured grid, which was used for the structural analysis, consisted of 14,440 hexahedral elements. The wall material was assumed to be hyperelastic, homogeneous, isotropic and nearly incompressible (Poisson ratio=0.45). According to experimental studies, the Young modulus of aortic wall was set equal to 4.66 MPa. The shear stress induced by the blood flow was neglected. A finite-element static structural analysis was performed. Three different cases were examined applying constant intraluminal systolic blood pressures of 120, 180 and 240 mmHg, respectively. The von Mises stress distribution and the displacements of the aortic wall were calculated. Peak wall stress for the normal load case of 120 mmHg was 22.5 N/cm2, while the max displacement was 0.44 mm. The case with the intraluminal pressure of 180 mmHg resulted into peak wall stress of 32 N/cm2 with max displacement 0.59 mm, while for 240 mmHg was 40.6N/cm2, max displacement 0.72 mm. The rise in blood pressure caused all stresses to increase. The pattern of stress distribution and the orientation of the stress were similar for all test cases. A quantitative evaluation of the aortic wall stresses under systolic hypertension is presented. The calculated values of peak wall stress are far lower to those of failure strength of healthy aortic wall specimens estimated by ex vivo mechanical testing (121.0 N/cm2). Our values are consistent with prior stress values predicted by experimental studies. The described methodology offers a significant advancement in incorporating biomechanical principles in the clinical assessment of hypertensive patients with normal or aneurysmatic aortas and can be applied in a patient-specific basis in both conditions in order to detect the vulnerable high stressed regions and the resultant risk of aortic dissection or rupture. We hypothesize that this could assist in deciding the timing of surgical intervention, especially in high-risk patients with abdominal aortic aneurysms.
计算心血管力学使科学家能够创建复杂的三维模型来模拟心血管问题。机械应力在心血管系统功能中起着关键作用;应力分析是理解血管病理生理学的有用工具。通过使用螺旋CT成像和计算结构分析,我们提出了一种在正常主动脉中进行壁应力分析的非侵入性方法。主动脉段从肠系膜下动脉起点延伸至主动脉分叉处。该段长度为12厘米,最大横向直径为2.075±0.129厘米。基于CT扫描图像构建了三维主动脉模型。假设主动脉壁厚度均匀,为1.5毫米。用于结构分析的生成的非结构化网格由14440个六面体单元组成。假设壁材料为超弹性、均匀、各向同性且近乎不可压缩(泊松比 = 0.45)。根据实验研究,将主动脉壁的杨氏模量设定为4.66兆帕。忽略血流引起的剪应力。进行了有限元静态结构分析。分别施加120、180和240毫米汞柱的恒定管腔内收缩期血压,检查了三种不同情况。计算了主动脉壁的冯·米塞斯应力分布和位移。120毫米汞柱正常负荷情况下的峰值壁应力为22.5牛/平方厘米,最大位移为0.44毫米。管腔内压力为180毫米汞柱的情况导致峰值壁应力为32牛/平方厘米,最大位移为0.59毫米,而对于240毫米汞柱,峰值壁应力为40.6牛/平方厘米,最大位移为0.72毫米。血压升高导致所有应力增加。所有测试情况的应力分布模式和应力方向相似。给出了收缩期高血压下主动脉壁应力的定量评估。计算得到的峰值壁应力值远低于通过体外力学测试估计的健康主动脉壁标本的破坏强度值(121.0牛/平方厘米)。我们的值与实验研究预测的先前应力值一致。所描述的方法在将生物力学原理纳入正常或动脉瘤性主动脉高血压患者的临床评估方面有了显著进展,并且可以在这两种情况下以患者特异性为基础应用,以检测易发生高应力的区域以及主动脉夹层或破裂的风险。我们假设这有助于确定手术干预的时机,特别是对于腹主动脉瘤的高危患者。