时变对流扩散方程的节点积分/有限元混合方法

Sundar Namala, R. Uddin
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引用次数: 0

摘要

节点积分法(NIM)是一类利用横向平均将控制偏微分方程(PDE)简化为一组常微分方程(ODE),并对这些常微分方程或其近似进行解析求解的高效粗网格方法。由于该方法依赖于横向平均,因此该方法的标准应用仅限于具有平行于坐标轴(2D)或坐标平面(3D)的边界的域。为了将节点积分/有限元混合方法扩展到任意领域,提出了节点积分/有限元混合方法。NI-FEM是基于内部区域和边界平行于坐标轴(2D)或坐标平面(3D)的区域可以用NIM求解,其余区域可以用FEM求解的思想。混合NI-FEM的关键是在NIM和FEM求解的区域之间的共同界面处建立界面条件。由于两种数值方法中的离散变量不同,因此需要对两种不同类型的离散元素之间的界面上的离散量进行特殊处理。本文报道了在Fortran的并行框架下,利用PETSc在任意域中求解随时间变化的对流扩散方程(CDE)的混合NI-FEM的发展。数值解与精确解的比较表明,该格式在空间和时间上都具有二阶精度。用于开发该方案的近似的阶数也显示为二阶。与传统的有限元法等独立数值格式相比,混合方法是有效的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Hybrid Nodal Integral/Finite Element Method (NI-FEM) for Time-Dependent Convection Diffusion Equation
Nodal integral methods (NIM) are a class of efficient coarse mesh method that use transverse averaging to reduce the governing partial differential equation(s) (PDE) into a set of ordinary differential equations (ODE), and these ODEs or their approximations are analytically solved. Since this method depends on transverse averaging, the standard application of this approach gets restricted to domains that have boundaries that are parallel to one of the coordinate axes (2D) or coordinate planes (3D). The hybrid nodal-integral/finite-element method (NI-FEM) has been developed to extend the application of NIM to arbitrary domains. NI-FEM is based on the idea that the interior region and the regions with boundaries parallel to the coordinate axes (2D) or coordinate planes (3D) can be solved using NIM and the rest of the domain can be solved using FEM. The crux of the hybrid NI-FEM is in developing interfacial conditions at the common interfaces between the regions solved by the NIM and the FEM. Since the discrete variables in the two numerical approaches are different, this requires special treatment of the discrete quantities on the interface between the two different types of discretized elements. We here report the development of hybrid NI-FEM in a parallel framework in Fortran using PETSc for the time-dependent convection-diffusion equation (CDE) in arbitrary domains. Numerical solutions are compared with exact solutions, and the scheme is shown to be second order accurate in both space and time. The order of approximations used for the development of the scheme are also shown to be second order. The hybrid method is efficient compared to standalone conventional numerical schemes like FEM.
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