Alagan Azhaganmaadevi K, Valeti Chanikya, Bolem Srinivas, Karve Omkar Sanjay, Arvind K R, Rajalakshmi P, Sabareeswaran A, Gopal Suraj, Matham Gowtham, Darshan H R, Sudhir B J, Patnaik B S V
Department of Applied Mechanics and Biomedical Engineering, Indian Institute of Technology Madras, Chennai, 600036, Tamil Nadu, India.
Department of Pathology, Sree Chitra Tirunal Institute for Medical Sciences and Technology, Trivandrum, 695011, Kerala, India.
Comput Biol Med. 2025 Feb;185:109579. doi: 10.1016/j.compbiomed.2024.109579. Epub 2024 Dec 26.
Cerebral aneurysms occur as balloon-like outpouchings in an artery, which commonly develop at the weak curved regions and bifurcations. When aneurysms are detected, understanding the risk of rupture is of immense clinical value for better patient management. Towards this, Fluid-Structure Interaction (FSI) studies can improve our understanding of the mechanics behind aneurysm initiation, progression, and rupture. Performing retrospective hemodynamic analysis using an accurate computational model that is closer to the actual biological milieu could yield clinically useful rupture risk predictions. Currently, the geometric model for the FSI studies rely on imaging the flow-domain using Computed Tomographic Angiography (CTA) or Digital Subtraction angiography (DSA), which limits accurate discerning of the vessel wall thickness. Histopathological information has always been ignored in accurately reconstructing the geometric model for the aneurysm. The present study combines both the shape information of the 3D lumen model (as it existed in vivo), which is accurately rendered through the CTA, in conjunction with the wall thickness information extracted from histo-pathological 2D images of the aneurysm. Furthermore, fluid-structure interaction (FSI) simulations are performed to understand the influence of patient-specific wall contribution towards rupture.
A 3D geometric model of the blood-flow domain of an anterior communicating artery (ACoA) aneurysm is extracted from the CTA of a patient that was surgically clipped. After safely clipping the aneurysm, the fundus of the aneurysm beyond the clip was cut and extracted. This was carefully preserved and sliced to obtain the wall thickness variation of the hoop at various axial sections. This study proposes a novel methodology of combining multi-modal image data to geometrically render the 3D model of the Cerebral aneurysm. The wall thickness extracted from the histological 2D cross-sectional images of the aneurysm is encapsulated around the 3D lumen model obtained from CT Angiographic data. To this end, a wall thickness transfer algorithm is developed to accurately reconstruct the patient-specific aneurysm wall thickness variation for the FSI simulations.
The wall thickness transfer algorithm accurately combines both the blood flow domain from the CT angiography and the histopathological images involving the wall thickness heterogeneity for the aneurysm. The patient-specific wall thickness variation, as it existed in vivo, has a mean wall thickness of 0.553 mm with a standard deviation of 0.256 mm. Detailed FSI simulations were performed to study the role of the patient-specific wall thickness (PWT) model vis-a-vis the uniform wall thickness (UWT) model. It was observed that the maximum wall stress for the UWT model was 13.6 kPa, while it was substantially higher for the PWT model (48.4 kPa). The maximum wall displacement for the UWT model was 58.5μm, while it was 162μm for the PWT model. Similarly, the mean wall stress for the UWT model was 2.13 kPa, while for the PWT model, it was 8.43 kPa. The mean wall displacement for the PWT model was substantially higher than the UWT model (52.58μm against 16.47μm).
The rendered patient-specific aneurysm wall model with its thickness variation, as it existed in vivo was obtained. Comparing fluid-structure interaction (FSI) simulation results, between the patient-specific wall-lumen combined model against the uniform wall thickness model have clearly shown that there were significant differences (p< 0.05) in the distribution of the hemodynamic parameters. The percentage difference in mean wall displacement and associated wall stress was 69% and 75%, respectively. Corresponding numbers for maximum wall displacement and maximum wall stress are 64% and 72%, respectively. Patient-specific fluid-structure interaction simulations show that, the present approach is highly valuable, as it improves our understanding towards rupture potential analysis for the cerebral aneurysms.
脑动脉瘤表现为动脉中呈气球样的向外膨出,通常在动脉的薄弱弯曲区域和分叉处形成。当检测到动脉瘤时,了解其破裂风险对于更好地管理患者具有巨大的临床价值。为此,流固耦合(FSI)研究可以增进我们对动脉瘤起始、发展和破裂背后力学机制的理解。使用更接近实际生物学环境的精确计算模型进行回顾性血流动力学分析,能够得出具有临床实用价值的破裂风险预测。目前,用于FSI研究的几何模型依赖于通过计算机断层血管造影(CTA)或数字减影血管造影(DSA)对血流区域进行成像,这限制了对血管壁厚度的精确辨别。在准确重建动脉瘤的几何模型时,组织病理学信息一直被忽视。本研究将通过CTA精确呈现的3D管腔模型(其在体内的形态)的形状信息与从动脉瘤的组织病理学二维图像中提取的壁厚信息相结合。此外,进行流固耦合(FSI)模拟以了解患者特异性血管壁对破裂的影响。
从一名接受手术夹闭的患者的CTA中提取前交通动脉(ACoA)动脉瘤血流区域的3D几何模型。在安全夹闭动脉瘤后,将夹子后方的动脉瘤底部切除并取出。小心保存并切片,以获得不同轴向截面处环向的壁厚变化。本研究提出了一种将多模态图像数据相结合以几何方式呈现脑动脉瘤3D模型的新方法。从动脉瘤的组织学二维横截面图像中提取的壁厚被封装在从CT血管造影数据获得的3D管腔模型周围。为此,开发了一种壁厚转移算法,以准确重建用于FSI模拟的患者特异性动脉瘤壁厚度变化。
壁厚转移算法准确地将CT血管造影的血流区域与涉及动脉瘤壁厚异质性的组织病理学图像相结合。患者特异性壁厚变化(其在体内的形态)的平均壁厚为0.553mm,标准差为0.256mm。进行了详细的FSI模拟,以研究患者特异性壁厚(PWT)模型相对于均匀壁厚(UWT)模型的作用。观察到UWT模型的最大壁应力为13.6kPa,而PWT模型的则显著更高(48.4kPa)。UWT模型的最大壁位移为58.5μm,而PWT模型的为162μm。同样,UWT模型的平均壁应力为2.13kPa,而PWT模型的为8.43kPa。PWT模型的平均壁位移显著高于UWT模型(分别为52.58μm和16.47μm)。
获得了呈现患者特异性动脉瘤壁模型及其在体内存在的厚度变化。比较患者特异性壁 - 管腔组合模型与均匀壁厚模型之间的流固耦合(FSI)模拟结果,清楚地表明血流动力学参数分布存在显著差异(p < 0.)。平均壁位移和相关壁应力的百分比差异分别为69%和75%。最大壁位移和最大壁应力的相应数字分别为64%和72%。患者特异性流固耦合模拟表明,本方法具有很高的价值,因为它增进了我们对脑动脉瘤破裂可能性分析的理解。