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True 2~(nd) Order Transmission Condition in Conjunction with Corner Edge Penalty Term for Non-conformal Domain Decomposition Methods in Solving Time-Harmonic Maxwell Equations

机译:真正的2〜(ND)订购传输条件与角落边缘惩罚术语用于解决时间谐波麦克风方程的非共形域分解方法

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Non-overlapping domain decomposition methods (DDMs) have been shown to provide efficient iterative algorithm for the finite element (FE) solution of the time-harmonic electromagnetic wave problems [1-4]. It is well known that the convergence behavior of non-overlapping DD methods is directly related to the transmission conditions (TCs) used to enforce the continuity of tangential fields on the interface between sub-domains. Most often, a 1st order complex Robin TC (FOTC) is used. However, by including higher order derivatives in the transverse direction, the convergence of iterative algorithms can be improved. In [3], a new type of SOTC, called SOTC-TE, is shown to considerably improve the convergence w.r.t. FOTC. But, it is only effective in preconditioning one set of problematic eigenvalues. The eigenmodes neglected by the SOTC-TE, namely the transverse magnetic (TM) evanescent modes, present the last impediment to solver convergence. We address these modes by introducing a full second-order TC (SOTC-Full) that includes an additional term with a second-order transverse derivative. An analysis using a simplified problem shows that, the SOTC-Full shifts both TE and TM evanescent eigen-values away from the origin, and does not alter the convergence of the propagating modes when compared to the FOTC. However, when the SOTC-Full is applied to non-conformal DDMs, it is quickly discovered that the performance does not achieve the expected speed-up as in the conformal DDMs. We have found that the root cause of such a defect, it is mainly due to the enlargement of the function space for the auxiliary cement variables on the interfaces, namely the use of the discontinuous curl-conforming basis functions for the auxiliary variables. Consequently, the non-conformal DDMs allow for eigen-modes, whose magnetic fluxes do not satisfy the needed divergence-free condition on the corner edges. To mitigate such a malady, we employ the interior penalty formulation and introduce additional corner penalty term relating to the divergence free constraint for the cement variables. The introduction of the corner edge penalty terms in the IP formulation restores the full benefits of the 2nd order TC in the non-conformal DDMs.
机译:已经示出了非重叠域分解方法(DDMS)为时间谐波电磁波问题的有限元(Fe)解决方案提供有效的迭代算法[1-4]。众所周知,非重叠DD方法的收敛行为与用于在子域之间的接口上执行切向字段的连续性的传输条件(TCS)直接相关。最常是使用1阶复合Robin TC(FOTC)。然而,通过在横向上包括高阶导数,可以提高迭代算法的收敛。在[3]中,新型的SOTC,称为SOTC-TE,显示为大大改善趋同w.r.t. FOTC。但是,它只有效地在预处理一组问题的特征值方面有效。由SOTC-TE忽略的特征模点,即横向磁性(TM)渐逝模式,呈现求解器收敛的最后障碍。我们通过引入完整的二阶TC(SOTC-Fuld)来解决这些模式,其中包括具有二阶横向导数的附加术语。使用简化问题的分析表明,SOTC-Full将TE和TM渐逝尖端值移除远离原点,并且与FOTC相比,不会改变传播模式的收敛。然而,当SOTC-FUNT应用于非共形DDMS时,很快发现性能不会达到与保形DDMS中的预期加速。我们已经发现这种缺陷的根本原因,主要是由于辅助水泥变量在接口上的函数空间的放大,即使用用于辅助变量的不连续的卷曲构成基函数。因此,非共形DDMS允许特征模式,其磁通量不满足在角边缘上的所需的无分歧状态。为了减轻这种疾病,我们采用内部惩罚制定,并引入与水泥变量的差异限制有关的额外的拐角惩罚术语。 IP配方中的拐角边缘惩罚术语的引入恢复了在非共形DDMS中的第二阶TC的全部益处。

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