Summation by parts methods for the spherical harmonic decomposition of the wave equation in arbitrary dimensions

Mathematics – Numerical Analysis

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Scientific paper

Splitting a solution of the wave equation in $n+1$ space dimensions into spherical harmonic components on $n$-spheres and reducing to first order results in the pair of first-order partial differential equations in radius and time $\dot\pi=\psi'+p\psi/r$ and $\dot\psi=\pi'$ for each spherical harmonic, where $p=2l+n$, and $l$ is a spherical harmonic index. The $\psi/r$ term gives rise to numerical stability problems near the origin, and also poses the key numerical difficulty in related systems of equations. We propose a class of summation by parts finite differencing methods that converge pointwise, including at $r=0$, and are stable because they admit a discrete energy. We explicitly construct such schemes that are 2nd and 4th order accurate at interior points, and first and 2nd order accurate at the spherical outer boundary $r=R$. We use the projection method to impose a class of boundary conditions for which the discrete energy is non-increasing.

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