介质体轴对称本征值问题

V. S. Bulygin, A. Vukovic, P. Sewell, T. Benson
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摘要

介质谐振器用于各种应用,包括滤波器,振荡器,频率计和调谐放大器。迄今为止,已经使用了一系列近似半解析方法来模拟微波介质谐振器,即磁壁法[1]、变分法[2]和各种积分方程方法[3,4]。特别有趣的是轮廓IE方法,它使用Muller IE和解析正则化方法(MAR)[5,6]将原始方程组转换为具有更有利特征的矩阵方程,即第二类Fredholm型方程。施加于椎间盘中间部分的条件[7]。我们的主要目标是在不做任何近似假设的情况下,将Muller IEs扩展到完整的3D情况。在本文中,我们提出了一个有价值的中间步骤,即基于Muller IE和旋转体(BOR)方法相结合的方法[4]。BOR方法是基于IE的方法,适用于具有轴(旋转)对称的物体,因此可以通过围绕对称轴旋转所谓的一般弧来获得。
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Axially symmetric eigenvalue problem for a dielectric body
Dielectric resonators are used in a variety of application, including filters, oscillators, frequencies meters and tuned amplifiers. To date, a range of approximate semi-analytical methods have been used to model microwave dielectric resonators, namely magnetic wall method [1], variational method [2], and various integral equation methods [3,4]. Of special interest are the contour IE methods that use the Muller IEs and the Method of Analytical Regularisation (MAR) [5,6] to convert the original equations set to the matrix equations with more favourable features, namely to the Fredholm type equations of the second kind.conditions imposed on the disk median section [7]. Our main objective is to extend the Muller IEs to the full 3D case without making any approximating assumptions. In this paper we present a valuable intermediate step, namely method based on the combination of Muller IE and the Body of Revolution (BOR) approach [4]. The BOR method is IE based method that is applicable to bodies that possess axial (rotational) symmetry and can thus be obtained by rotating a so-called generic arc around the axis of symmetry.
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