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通过计算流体动力学分析确定脑动脉瘤破裂点的局部血液动力学。

Local hemodynamics at the rupture point of cerebral aneurysms determined by computational fluid dynamics analysis.

机构信息

Departments of Neurosurgery, Tohoku University Graduate School of Medicine, Sendai, Japan.

出版信息

Cerebrovasc Dis. 2012;34(2):121-9. doi: 10.1159/000339678. Epub 2012 Aug 1.

Abstract

BACKGROUND

Cerebral aneurysms carry a high risk of rupture and so present a major threat to the patient's life. Accurate criteria for predicting aneurysm rupture are important for therapeutic decision-making, and some clinical and morphological factors may help to predict the risk for rupture of unruptured aneurysms, such as sex, size and location. Hemodynamic forces are considered to be key in the natural history of cerebral aneurysms, but the effect on aneurysm rupture is uncertain, and whether low or high wall shear stress (WSS) is the most critical in promoting rupture remains extremely controversial. This study investigated the local hemodynamic features at the aneurysm rupture point.

METHODS

Computational models of 6 ruptured middle cerebral artery aneurysms with intraoperative confirmation of rupture point were constructed from 3-dimensional rotational angiography images. Computational fluid dynamics (CFD) simulations were performed under pulsatile flows using patient-specific inlet flow conditions. Time-averaged WSS (TAWSS) and oscillatory shear index (OSI) were calculated, and compared at the rupture point and at the aneurysm wall without the rupture point. We performed an additional CFD simulation of a bleb-removed model for a peculiar case in which bleb formation could be confirmed by magnetic resonance angiography.

RESULTS

All rupture points were located at the body or dome of the aneurysm. The TAWSS at the rupture point was significantly lower than that at the aneurysm wall without the rupture point (1.10 vs. 4.96 Pa, p = 0.031). The OSI at the rupture point tended to be higher than at the aneurysm wall without the rupture point, although the difference was not significant (0.0148 vs. 0.0059, p = 0.156). In a bleb-removed simulation, the TAWSS at the bleb-removed area was 6.31 Pa, which was relatively higher than at the aneurysm wall (1.94 Pa).

CONCLUSION

The hemodynamics of 6 ruptured cerebral aneurysms of the middle cerebral artery were examined using retrospective CFD analysis. We could confirm the rupture points in all cases. With those findings, local hemodynamics of ruptured aneurysms were quanti-tatively investigated. The rupture point is located in a low WSS region of the aneurysm wall. Bleb-removed simulation showed increased WSS of the bleb-removed area, associated with the flow impaction area. Although the number of subjects in this study was relatively small, our findings suggest that the location of the rupture point is related to a low WSS at the aneurysm wall. Further investigations will elucidate the detailed hemodynamic effects on aneurysm rupture.

摘要

背景

脑动脉瘤破裂风险很高,因此对患者的生命构成重大威胁。准确预测动脉瘤破裂的标准对于治疗决策很重要,一些临床和形态学因素可能有助于预测未破裂动脉瘤的破裂风险,例如性别、大小和位置。血流动力学力被认为是脑动脉瘤自然史中的关键因素,但对动脉瘤破裂的影响尚不确定,低壁切应力(WSS)还是高壁切应力最能促进破裂仍然存在很大争议。本研究调查了动脉瘤破裂点的局部血流动力学特征。

方法

从术中确认破裂点的 3 个三维旋转血管造影图像中构建了 6 个破裂的大脑中动脉动脉瘤的计算模型。使用患者特定的入口流量条件在脉动流下进行计算流体动力学(CFD)模拟。计算破裂点和无破裂点动脉瘤壁处的时均壁切应力(TAWSS)和振荡剪切指数(OSI),并进行比较。我们对磁共振血管造影可确认形成小泡的特殊病例进行了额外的 CFD 模拟。

结果

所有破裂点均位于动脉瘤的体部或瘤顶。破裂点处的 TAWSS 明显低于无破裂点处的 TAWSS(1.10 比 4.96 Pa,p = 0.031)。破裂点处的 OSI 趋于高于无破裂点处的 OSI,尽管差异无统计学意义(0.0148 比 0.0059,p = 0.156)。在小泡去除模拟中,小泡去除区域的 TAWSS 为 6.31 Pa,相对高于动脉瘤壁(1.94 Pa)。

结论

使用回顾性 CFD 分析检查了 6 个大脑中动脉破裂动脉瘤的血流动力学。我们可以在所有病例中确认破裂点。通过这些发现,定量研究了破裂动脉瘤的局部血流动力学。破裂点位于动脉瘤壁的低 WSS 区域。小泡去除模拟显示,小泡去除区域的 WSS 增加,与流撞击区域相关。尽管本研究的研究对象数量相对较少,但我们的研究结果表明,破裂点的位置与动脉瘤壁的低 WSS 有关。进一步的研究将阐明动脉瘤破裂的详细血流动力学影响。

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