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首页> 外文期刊>IEEE Transactions on Antennas and Propagation >Finite-Element Time-Domain Solution of the Vector Wave Equation in Doubly Dispersive Media Using M?bius Transformation Technique
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Finite-Element Time-Domain Solution of the Vector Wave Equation in Doubly Dispersive Media Using M?bius Transformation Technique

机译:基于M?bius变换技术的双色散介质中矢量波方程的时域有限元求解

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Several finite-element time-domain (FETD) formulations to model inhomogeneous and electrically/magnetically/doubly dispersive materials based on the second-order vector wave equation discretized by the Newmark-$beta $ scheme are developed. In contrast to the existing formulations, which employ recursive convolution (RC) approaches, we use a Möbius transformation method to derive our new formulations. Hence, the obtained equations are not only simpler in form and easier to derive and implement, but also do not suffer from the intrinsic limitations of the RC methods in modeling arbitrary high-order media. To obtain the formulations, we first demonstrate that the update equation for the electric field strength ${e}$ in the mixed Crank-Nicolson (CN) FETD formulation, which is based on expanding the electric and magnetic field in terms of the edge and face elements in space and discretizing the resultant first-order differential equations using Crank-Nicolson scheme in time, is equivalent to the unconditionally stable (US) second-order vector wave equation for the same variable (${e}$) discretized by the Newmark-$beta $ method with $beta =1/4$. In addition, we show that the update equation for the magnetic flux density ${b}$ in CN-FETD is the same as the second-order vector wave equation for ${b}$ on the dual grid discretized again by a similar Newmark-$beta $ method.
机译:几种有限元时域(FETD)公式,用于基于由Newmark- $ beta $ 方案。与采用递归卷积(RC)方法的现有公式相反,我们使用Möbius变换方法来导出我们的新公式。因此,所获得的方程不仅形式更简单,更易于推导和实现,而且不受RC方法在任意高阶介质建模中的固有局限性的困扰。为了获得公式,我们首先证明了混合曲柄中电场强度的更新公式 $ {e} $ -Nicolson(CN)FETD公式基于空间中的边缘和面元素扩展电场和磁场,并及时使用Crank-Nicolson方案离散化所得的一阶微分方程,该公式等效于无条件由Newmark-离散化的相同变量( $ {e} $ )的稳定(美国)二阶矢量波方程 $ beta $ 方法与 $ beta = 1 / 4 $ 。另外,我们表明,CN-FETD中的磁通密度 $ {b} $ 的更新方程是相同的作为二元网格上 $ {b} $ 的二阶矢量波方程,再次由类似的Newmark- <公式Formulatype =“ inline”> $ beta $ 方法。

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