A hybrid surface integral equation partial differential equation (SIE-PDE) formulation without the boundary condition requirement is proposed to solve the electromagnetic problems. In the proposed formulation, the computational domain is decomposed into two \emph{overlapping} domains: the SIE and PDE domains. In the SIE domain, complex structures with piecewise homogeneous media, e.g., highly conductive media, are included. An equivalent model for those structures is constructed through replacing them by the background medium and introducing a surface equivalent electric current density on an enclosed boundary to represent their electromagnetic effects. The remaining computational domain and homogeneous background medium replaced domain consist of the PDE domain, in which inhomogeneous or non-isotropic media are included. Through combining the surface equivalent electric current density and the inhomogeneous Helmholtz equation, a hybrid SIE-PDE formulation is derived. Unlike other hybrid formulations, where the transmission condition is usually used, no boundary conditions are required in the proposed SIE-PDE formulation, and it is mathematically equivalent to the original physical model. Through careful construction of basis functions to expand electric fields and the equivalent current density, the discretized formulation is compatible on the interface of the SIE and PDE domain. Finally, its accuracy and efficiency are validated through two numerical examples. Results show that the proposed SIE-PDE formulation can obtain accurate results including both near and far fields, and significant performance improvements in terms of CPU time and memory consumption compared with the FEM are achieved.
翻译:为了解决电磁问题,建议采用没有边界条件要求的混合表面整体方程式(SIE-PDE)部分差异方程(SIE-PDE)配方,以解决电磁问题。在拟议的配方中,计算域被分解成两个\emph{overplay}域:SIE和PDE域。在SIE域中,包含一个具有片面等效同同质介质的复杂结构,例如高导导电介质等同质介质。通过用背景介质替换这些结构,并在封闭边界中引入一个表面等同的电流密度以表示其电磁效应。其余的计算域和同质背景介质替代域由PDE域组成,其中包含不相形或非异的介质介质介质。通过对表面等电密度密度和不相容的电离异性介质结构,SIE-PDE域域的精确度和直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直径直、直直径直径直直直直直直径直直直直直直直径直直直直直直径直直直直直直直直直直直直直直直直直直直直直直直距直直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距直距