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Summation by parts methods for spherical harmonic decompositions of the wave equation in any dimensions

机译:任何维数波动方程的球谐分解的分部求和方法

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We investigate numerical methods for wave equations in n + 2 spacetime dimensions, written in spherical coordinates, decomposed in spherical harmonics on Sn, and finite-differenced in the remaining coordinates r and t. Such an approach is useful when the full physical problem has spherical symmetry, for perturbation theory about a spherical background, or in the presence of boundaries with spherical topology. The key numerical difficulty arises from lower order 1/r terms at the origin r = 0. As a toy model for this, we consider the flat space linear wave equation in the form,, where p = 2l + n and l is the leading spherical harmonic index. We propose a class of summation by parts (SBP) finite-differencing methods that conserve a discrete energy up to boundary terms, thus guaranteeing stability and convergence in the energy norm. We explicitly construct SBP schemes that are second- and fourth-order accurate at interior points and the symmetry boundary r = 0, and first- and second-order accurate at the outer boundary r = R.
机译:我们研究了n + 2时空维度中波动方程的数值方法,用球坐标表示,在Sn上分解为球谐函数,并在其余坐标r和t中进行有限差分。当完整的物理问题具有球形对称性,关于球形背景的扰动理论或存在球形拓扑边界时,这种方法很有用。关键的数值困难是由原点r = 0处的低阶1 / r项引起的。为此,作为玩具模型,我们考虑以下形式的平面空间线性波动方程,其中p = 2l + n并且l为前导球谐指数。我们提出了一类按部分求和(SBP)的有限差分方法,该方法可以将离散能量保存到边界项,从而保证能量范数的稳定性和收敛性。我们显式构造了SBP方案,这些方案在内部点和对称边界r = 0时是二阶和四阶精度,在外部边界r = R时是一阶和二阶精度。

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