2019
DOI: 10.1155/2019/8532408
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A Robust Optimal Finite Difference Scheme for the Three‐Dimensional Helmholtz Equation

Abstract: We propose a robust optimal 27-point finite difference scheme for the Helmholtz equation in three-dimensional domain. In each direction, a special central difference scheme with 27 grid points is developed to approximate the second derivative operator. The 27 grid points are divided into four groups, and each group is involved in the difference scheme by the manner of weighted combination. As for the approximation of the zeroth-order term, we use the weighted average of all the 27 points, which are also divide… Show more

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Cited by 7 publications
(4 citation statements)
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References 31 publications
(45 reference statements)
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“…It is shown that the numerical results are in good agreement with the analytical ones. The third example [68] is…”
Section: Numerical Examplesmentioning
confidence: 99%
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“…It is shown that the numerical results are in good agreement with the analytical ones. The third example [68] is…”
Section: Numerical Examplesmentioning
confidence: 99%
“…The CPU times of the IEFG method and the EFG method are 200.6 s and 208.1 s, respectively. The third example [68] is ∆u + k 2 u = (k 2 − 3π 2 ) cos(πx 1 ) sin(πx 2 ) sin(πx 3 ).…”
Section: Numerical Examplesmentioning
confidence: 99%
“…In order to suppress the "pollution effect" and reduce the numerical dispersion, many numerical methods have been proposed in the past decades (cf. [1,2,[15][16][17][18][19]).…”
Section: Introductionmentioning
confidence: 99%
“…In [6], an optimal 9point difference scheme is developed, which is consistent with the Helmholtz equation with perfectly matched layer (PML). To improve the robustness, the authors of [7,16] established robust optimal difference schemes which works efficiently even if the step sizes along different directions are not equal. To reduce the numerical error, higher-order finite difference schemes (cf.…”
Section: Introductionmentioning
confidence: 99%