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Wavelets and convolution quadrature for the efficient solution of a 2D space-time BIE for the wave equation

机译:波动方程的2D时空偏见的高效解的小波和卷积正交

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We consider a wave propagation problem in 2D, reformulated in terms of a Boundary Integral Equation (BIE) in the space-time domain. For its solution, we propose a numerical scheme based on a convolution quadrature formula by Lubich for the discretization in time, and on a Galerkin method in space. It is known that the main advantage of Lubich's formulas is the use of the FFT algorithm to retrieve discrete time integral operators with a computational complexity of order R log R, R being twice the total number of time steps performed. Since the discretization in space leads in general to a quadratic complexity, the global computational complexity is of order (MR)-R-2 log R and the working storage required is (MR)-R-2/2, where M is the number of grid points on the domain boundary.
机译:我们考虑2D中的波传播问题,在空时域中的边界积分方程(BIE)方面重新计算。 对于其解决方案,我们提出了一种基于Lubich的卷积正交公式的数值方案,以便在时间上分离,以及在空间中的Galerkin方法。 众所周知,Lubich的公式的主要优点是使用FFT算法来检索具有顺序R Log R的计算复杂度的离散时间积分运算符,R是执行的总时间步骤的两倍。 由于空间中的离散化通用于二次复杂性,因此全局计算复杂性是顺序(MR)-R-2 log R,并且所需的工作存储是(MR)-R-2/2,其中M是数字 域边界网格点。

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