The scattering of electromagnetic waves from obstacles with wave-material interaction in thin layers on the surface is described by generalized impedance boundary conditions, which provide effective approximate models. In particular, this includes a thin coating around a perfect conductor and the skin effect of a highly conducting material. The approach taken in this work is to derive, analyse and discretize a system of time-dependent boundary integral equations that determines the tangential traces of the scattered electric and magnetic fields. In a familiar second step, the fields are evaluated in the exterior domain by a representation formula, which uses the time-dependent potential operators of Maxwell's equations. The time-dependent boundary integral equationis discretized with Runge--Kutta based convolution quadrature in time and Raviart--Thomas boundary elements in space. Using the frequency-explicit bounds from the well-posedness analysis given here together with known approximation properties of the numerical methods, the full discretization is proved to be stable and convergent, with explicitly given rates in the case of sufficient regularity. Taking the same Runge--Kutta based convolution quadrature for discretizing the time-dependent representation formulas, the optimal order of convergence is obtained away from the scattering boundary, whereas an order reduction occurs close to the boundary. The theoretical results are illustrated by numerical experiments.
翻译:电磁波从地表薄层中波状物质相互作用的屏障中散落的电磁波在表面薄质层中,其描述是普遍的阻隔边界条件,这些条件提供了有效的近似模型,特别是,这包括围绕一个完美的导体的薄层涂层,以及高度进行材料的皮肤效应。这项工作采取的方法是产生、分析和分解一个时间依赖的边界整体方程式系统,这个系统将决定分散的电磁场和磁场的相近痕迹。在熟悉的第二步中,用一个代表公式在外部领域对字段进行评价,该公式使用马克斯韦尔方程式中的时间依赖的潜在操作者。基于时间的取决于时间的边界整体方程式与基于Runge-Kuta的卷变二次曲线和空间Raviart-Thoomas的边界元素分离。利用此处对远端电磁场和磁场的已知近似特性进行的频度分析所显示的界限界限界限,完全离散化被证明是稳定和趋同的,在足够固定的情况下,明确给出了速度。以同样的Renge-Kut为基基基的圆形组合组合分解,从空间的离离离面的公式,而从最接近的边界分解的公式则从最接近的分解的公式,从最接近的边界分解的分解的公式是分解。