基于格子Boltzmann方法的個(gè)體化顱內(nèi)動(dòng)脈瘤幾何重建及其數(shù)值模擬
[Abstract]:Intracranial aneurysms are one of the most dangerous and common diseases that endanger human health. Hemodynamics, as a major factor affecting the generation, development, rupture and treatment of intracranial aneurysms, has attracted wide attention of scholars both at home and abroad. In clinical treatment, interventional therapy with blood flow diversion stent and coil embolization has been achieved. However, the traditional clinical trials are faced with the difficulties of high risk, long cycle and high cost. At present, individual numerical experiments based on medical images are favored. Most of the existing numerical methods use various computational flows. Body mechanics (CFD) software is limited by the complex geometry of blood vessels, the characteristics of blood flow and the low computational efficiency.
In recent years, lattice Boltzmann method (LBM) has attracted more and more attention because of its rapid development in computational fluid dynamics. LB method has its natural advantages in the generality of models, the ability to deal with complex boundaries and the efficiency of computation. It is suitable for the simulation and analysis of intracranial aneurysm hemodynamics. As an effective numerical method, the method is used to solve various partial differential equations, such as convection-diffusion equation, reaction-diffusion equation and Poisson equation.
At present, there are some research work on the numerical simulation of aneurysm hemodynamics based on LBM, but most of the work on the geometric model of aneurysm is based on the two-dimensional model or the ideal three-dimensional model combined with cylinder and sphere, lacking of individual patient research; in the study of individual patient data, the import and export of numerical simulation. On this basis, the whole process of individualized hemodynamic simulation of intracranial aneurysms is studied by using LBM as the main numerical means: starting from the clinical acquired three-dimensional tomographic medical image data, a variety of lattice Boltzmann models are developed and implemented with the help of a graphics processor (GPU) parallel computing device. Individual patient's blood vessel image segmentation, geometric reconstruction, LBM computational grid processing and hemodynamics simulation.
The work of this paper includes two aspects: reconstruction of the geometric shape of aneurysm and numerical simulation of hemodynamics with complex boundary.
(1) By studying the characteristics of the lattice Boltzmann method and the image denoising, edge detection and image segmentation model based on PDE, this paper proposes a LB model which can efficiently solve image denoising, edge detection and image segmentation, and applies this model to the computed tomography image of intracranial aneurysms. In principle, the 3D geometric model of individual aneurysms can be accurately segmented. The model can not only be applied to medical images, but also has a good effect on contour detection and image segmentation of more complex natural images.
(2) In order to meet the needs of grid computing and clinical research, we have further improved the geometric model to make the geometric model more reasonable. Based on the results of image segmentation, we propose a vascular center line method to reconstruct tumor-bearing vessels and vascular stents. On the other hand, the branches near the aneurysms can be freely removed according to the needs of the study. Compared with the three-dimensional models reconstructed by traditional CFD software, the geometric model presented in this paper is more reasonable and can meet the design of various types of vascular stents.
In the numerical simulation of complex boundary hemodynamics,
(1) Based on the vascular geometry model, we developed a lattice Boltzmanr model with complex boundary to solve the Navier-Stokes equations describing hemodynamics. We also discussed the individualized inlet and outlet conditions of intracranial aneurysms. In addition, under the boundary conditions of the velocity inlet and the pressure outlet, the difference between the pulsatile velocity inlet and the steady velocity inlet is discussed. It is found that the flow state at the peak time of the pulsatile flow can be approximately simulated by using the mean value of the pulsatile velocity and the mean value of the pulsatile peak value as the steady velocity inlet.
(2) Combining with the problems in clinical treatment, we simulated the data of several patients with carotid aneurysms. Aiming at the design of stents, we studied the hemodynamic changes in aneurysms after implantation of different dense and different types of stents. With the increase of stent density, the same dense spiral mesh stent can inhibit the intratumoral velocity more effectively than single spiral stent. The effect of the branches near the aneurysm on the intratumoral hemodynamics was studied, and the velocity and flow pattern inside the aneurysm were analyzed. The flow field in the aneurysm is smaller when the diameter of the branch is larger or the branch is farther away from the aneurysm.
In a word, this paper takes the lattice Boltzmann method as the main numerical means, establishes the whole scheme of individual intracranial aneurysm hemodynamics simulation, and completes the design of LB algorithm under the high performance parallel platform of GPU. Compared with the CPU program, the acceleration ratio of nearly two orders of magnitude is obtained, which greatly improves the efficiency of numerical simulation algorithm. In order to further explore the treatment of aneurysms, two kinds of spiral stents were digitally implanted into the geometric models of individual patients with aneurysms. On the one hand, the numerical models were used. This paper provides a theoretical explanation for the clinical treatment, on the other hand, it provides guidance for the selection and placement of clinical vascular stents.
【學(xué)位授予單位】:華中科技大學(xué)
【學(xué)位級(jí)別】:博士
【學(xué)位授予年份】:2014
【分類號(hào)】:TP391.41;R739.41
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