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首页> 外文期刊>Journal of Computational Physics >An adaptive meshfree method for phase-field models of biomembranes. Part I: Approximation with maximum-entropy basis functions
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An adaptive meshfree method for phase-field models of biomembranes. Part I: Approximation with maximum-entropy basis functions

机译:一种适用于生物膜相场模型的自适应无网格方法。第一部分:具有最大熵基函数的逼近

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摘要

We present an adaptive meshfree method to approximate phase-field models of biomembranes. In such models, the Helfrich curvature elastic energy, the surface area, and the enclosed volume of a vesicle are written as functionals of a continuous phase-field, which describes the interface in a smeared manner. Such functionals involve up to second-order spatial derivatives of the phase-field, leading to fourth-order Euler-Lagrange partial differential equations (PDE). The solutions develop sharp internal layers in the vicinity of the putative interface, and are nearly constant elsewhere. Thanks to the smoothness of the local maximum-entropy (max-ent) meshfree basis functions, we approximate numerically this high-order phase-field model with a direct Ritz-Galerkin method. The flexibility of the meshfree method allows us to easily adapt the grid to resolve the sharp features of the solutions. Thus, the proposed approach is more efficient than common tensor product methods (e.g. finite differences or spectral methods), and simpler than unstructured C0 finite element methods, applicable by reformulating the model as a system of second-order PDE. The proposed method, implemented here under the assumption of axisymmetry, allows us to show numerical evidence of convergence of the phase-field solutions to the sharp interface limit as the regularization parameter approaches zero. In a companion paper, we present a Lagrangian method based on the approximants analyzed here to study the dynamics of vesicles embedded in a viscous fluid.
机译:我们提出了一种自适应无网格方法来近似生物膜的相场模型。在这样的模型中,海夫里希曲率弹性能,表面积和囊泡的封闭体积被写为连续相场的函数,该相场以涂抹的方式描述了界面。这种泛函涉及相位场的二阶空间导数,从而导致四阶欧拉-拉格朗日偏微分方程(PDE)。这些解决方案在假定的界面附近形成了尖锐的内层,而在其他地方几乎保持不变。由于局部最大熵(max-ent)无网格基函数的平滑性,我们使用直接的Ritz-Galerkin方法在数值上近似了此高阶相场模型。无网格方法的灵活性使我们能够轻松调整网格以解决解决方案的尖锐特性。因此,所提出的方法比普通的张量积方法(例如有限差分或谱方法)更有效,并且比非结构化的C0有限元方法更简单(可通过将模型重新构造为二阶PDE系统来应用)。此处提出的方法是在轴对称性的假设下实施的,它使我们能够显示出当正则化参数趋近于零时,相场解收敛到尖锐的界面极限的数值证据。在随附的论文中,我们基于本文分析的近似值提出了一种拉格朗日方法,以研究嵌入在粘性流体中的囊泡的动力学。

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