用奇异积分方程计算微带线

V. Ivashka, Ju. Lauchius, V. Shugurov
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引用次数: 0

摘要

在均匀填充情况下,微带线中最低模式的电磁场是横向的,可以用谐波函数来描述。如果填充是分段均匀的,则低频产生的电场和磁场的纵向分量远小于横向分量。这允许我们使用横向电磁波的近似。所提出的方法的思想是以柯西型积分的形式来表示势。从而满足微分方程。然后边界条件得到奇异积分方程[1]。我们过去常用数值方法解方程。在一些最简单的情况下,有可能得到解析形式的解。该方法的主要优点是:1 .该方法将二维问题的求解简化为一维问题的求解,大大缩短了计算机时间。2. 解的算法和方程的形式不依赖于直线截面的形状。3.解在角点上的行为与静态行为严格对应。4. 从计算的角度来看,将该方法应用于具有实际几何尺寸的线(例如有限厚度的条)似乎更方便。如果考虑一条具有无限细条的直线,则可以方便地使用Muskhelishvili的表示
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Calculation of Microstrip Lines by Means of Singular Integral Equations
In case of homogeneous filling the electromagnetic field of the lowest mode in a microstrip line is transverse and can be described by harmonic functions. If the filling is piecewise homogeneous the longitudinal components of electric and magnetic fields arise for lower frequencies being much less than transverse ones. This allows one to use the approximation of transverse electromagnetic waves. The idea of the proposed method is to represent the potential in the form of a Cauchy type integral. Thus the differential equations are satisfied. Then the boundaryr conditions lead to singular integral equations [ I]. We used to solve the equations numerically. In some simplest cases it is possible to get a solution in an analytical form. The main advantages of a method are: I. The method reduces the solution of a two-dimensional problem to one-dimensional one drasticadly shortening computer time. 2. The algorithm of the solution and the form of the equations don't depend on the shape of the line cross section. 3. The conduct of the solution in angular points rigorously corresponds to the static one. 4. From the computational point of view it appeared to be more convenient to apply the method to the line having real geometrical sizes (say finite thickness of a strip). If one considers a line having infinitely thin strips it is convenient to use the representation by Muskhelishvili
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