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On energy stable discontinuous Galerkin spectral element approximations of the perfectly matched layer for the wave equation

机译:波动方程完美匹配层的能量稳定非连续Galerkin谱元素逼近

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In this paper, we develop a provably energy stable discontinuous Galerkin spectral element method (DGSEM), approximating the perfectly matched layer (PML) for the three and two space dimensional (3D and 2D) linear acoustic wave equations, in first order form, subject to well-posed linear boundary conditions. First, using the well-known complex coordinate stretching, we derive an efficient un-split modal PML for the 3D acoustic wave equation, truncating a cuboidal computational domain. Second, we prove asymptotic stability of the continuous PML by deriving energy estimates in the Laplace space, for the 3D PML in a heterogeneous acoustic medium, assuming piece-wise constant PML damping. In the time-domain, the energy estimate translates to a bound for the solutions in terms of the initial data. Third, we develop a DGSEM for the wave equation using physically motivated numerical flux, with penalty weights, which are compatible with all well-posed, internal and external, boundary conditions. When the PML damping vanishes, by construction, our choice of penalty parameters yields an upwind scheme and a discrete energy estimate analogous to the continuous energy estimate. Fourth, to ensure numerical stability of the discretization when PML is present, it is necessary to systematically extend the numerical fluxes, and the inter-element and boundary procedures, to the PML auxiliary differential equations. This is critical for deriving discrete energy estimates analogous to the continuous energy estimates. Finally, we propose a procedure to compute PML damping coefficients such that the PML error converges to zero, at the optimal convergence rate of the underlying numerical method. Numerical solutions are evolved in time using the high order Taylor-type time stepping scheme of the same order of accuracy of the spatial discretization. By combining the DGSEM spatial approximation with the high order Taylor-type time stepping scheme and the accuracy of the PML we obtain an arbitrarily accurate wave propagation solver in the time domain. Numerical experiments are presented in 2D and 3D corroborating the theoretical results. (C) 2019 The Authors. Published by Elsevier B.V.
机译:在本文中,我们开发了一种可证明的能量稳定的不连续伽勒金谱元方法(DGSEM),以一阶形式逼近了三维空间二维声波方程(3D和2D)的完美匹配层(PML)。到适当的线性边界条件首先,使用众所周知的复数坐标拉伸,我们为3D声波方程式导出了有效的非分裂模态PML,将立方计算域截断了。其次,我们假设3D PML在非均匀声学介质中,假设分段恒定PML阻尼,通过推导Laplace空间中的能量估计来证明连续PML的渐近稳定性。在时域中,能量估计转化为初始数据方面的解的界线。第三,我们使用物理数值通量和波动权重开发了波动方程的DGSEM,该权重与所有适当摆放的内部和外部边界条件兼容。当PML阻尼消失时,通过构造,我们选择的惩罚参数会产生上风方案和类似于连续能量估计的离散能量估计。第四,为了确保存在PML时离散化的数值稳定性,有必要将数值通量以及元素间和边界过程扩展到PML辅助微分方程。这对于得出类似于连续能量估算值的离散能量估算值至关重要。最后,我们提出了一种程序来计算PML阻尼系数,以使PML误差以基本数值方法的最佳收敛速度收敛到零。数值解决方案是使用与空间离散化精度相同的高阶泰勒式时间步进方案随时间演化的。通过将DGSEM空间逼近与高阶泰勒式时间步进方案和PML的精度相结合,我们获得了时域中任意精确的波传播求解器。在2D和3D中进行了数值实验,证实了理论结果。 (C)2019作者。由Elsevier B.V.发布

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