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Generalization of the Second Order Vector Potential Formulation for Arbitrary Non-Orthogonal Curvilinear Coordinates Systems from the Covariant Form of Maxwell's Equations

机译:麦克斯韦方程组协变形式的任意非正交曲线坐标系二阶矢量势公式的推广

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A great number of semi-analytical models, notably the representation of electromagnetic fields by integral equations are based on the second order vector potential (SOVP) formalism which introduces two scalar potentials in order to obtain analytical expressions of the electromagnetic fields from the two potentials. However, the scalar decomposition is often known for canonical coordinate systems. This paper aims in introducing a specific SOVP formulation dedicated to arbitrary non-orthogonal curvilinear coordinates systems. The electromagnetic field representation which is derived in this paper constitutes the key stone for the development of semi-analytical models for solving some eddy currents moelling problems and electromagnetic radiation problems considering at least two homogeneous media separated by a rough interface. This SOVP formulation is derived from the tensor formalism and Maxwell’s equations written in a non-orthogonal coordinates system adapted to a surface characterized by a 2D arbitrary aperiodic profile.
机译:大量的半分析模型,特别是通过积分方程表示的电磁场,是基于二阶矢量势(SOVP)形式主义的,它引入了两个标量势,以便从两个势中获得电磁场的解析表达式。但是,标量分解对于规范坐标系通常是已知的。本文旨在介绍专用于任意非正交曲线坐标系的特定SOVP公式。本文得出的电磁场表示法是开发半解析模型的关键石,该半解析模型用于解决考虑至少两个被粗糙界面分开的均匀介质的涡流熔融问题和电磁辐射问题。这种SOVP公式是从张量形式主义和麦克斯韦方程组衍生而来的,该方程写在非正交坐标系中,该坐标系适用于以2D任意非周期性轮廓为特征的表面。

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