On accuracy conditions for the numerical computation of waves
The Helmholtz equation ( Δ+ K 2 n 2) u= f with a variable index of refraction n and a suitable radiation condition at infinity serves as a model for a wide variety of wave propagation problems. Such problems can be solved numerically by first truncating the given unbounded domain, imposing a suitabl...
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Veröffentlicht in: | J. Comput. Phys.; (United States) 1985-07, Vol.59 (3), p.396-404 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The Helmholtz equation (
Δ+
K
2
n
2)
u=
f with a variable index of refraction
n and a suitable radiation condition at infinity serves as a model for a wide variety of wave propagation problems. Such problems can be solved numerically by first truncating the given unbounded domain, imposing a suitable outgoing radiation condition on an artificial boundary and then solving the resulting problem on the bounded domain by direct discretization (for example, using a finite element method). In practical applications, the mesh size
h and the wave number
K are not independent but are constrained by the accuracy of the desired computation. It will be shown that the number of points per wavelength, measured by (
Kh)
−1, is not sufficient to determine the accuracy of a given discretization. For example, the quantity
K
3
h
2 is shown to determine the accuracy in the
L
2 norm for a second-order discretization method applied to several propagation models. |
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ISSN: | 0021-9991 1090-2716 |
DOI: | 10.1016/0021-9991(85)90119-6 |