Nonreflecting Boundary Kernels

The exact nonreflecting boundary conditions are derived from separation of variables in rectangular, cylindrical, or spherical coordinate systems. Under this separation, the boundary condition for each wavenumber is independent of the others, and depends on its own history by a convolution. The convolution kernels in the Laplace domain for three different wavenumbers are shown in the plot below.
Real and imaginary parts of various convolution kernels are plotted on the imaginary axis.
The plot shows the real and imaginary parts of the kernels on the imaginary axis. (For each, the real part is even.) The simplicity of these kernels leads their efficient approximation as rational functions, with controlled (arbitrarily small) error.

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Bradley K Alpert
Last modified: Fri Jul 14 12:11:53 MDT 2000