2010
DOI: 10.1016/j.jcp.2010.04.011
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Coupling of Dirichlet-to-Neumann boundary condition and finite difference methods in curvilinear coordinates for multiple scattering

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Cited by 26 publications
(41 citation statements)
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“…This provides a very convenient way when one does not want to use the specific functions or need to build a more complicated operator. For example, the spectral (dense) construction of the BWIE for the Dirichlet problem can be written IntegralOperator(O, a, M modes, k, [1,2,3], [0.5, -eta, -1]);…”
Section: Defining and Solving An Integral Equationmentioning
confidence: 99%
See 1 more Smart Citation
“…This provides a very convenient way when one does not want to use the specific functions or need to build a more complicated operator. For example, the spectral (dense) construction of the BWIE for the Dirichlet problem can be written IntegralOperator(O, a, M modes, k, [1,2,3], [0.5, -eta, -1]);…”
Section: Defining and Solving An Integral Equationmentioning
confidence: 99%
“…The vector M modes is such that M modes(p)= N p , the argument vector [1,2,3] refers to respectively the operators Identity (1), L (2) and M (3) and the last one [0.5, -eta, -1] carries the weight to apply to each operator in the linear combination (eta must previously have taken a prescribed complex value in the script). Without entering too much into details, each block of the final global matrix can be specified thanks to this numbering (instead of a vector, a 2D-or a 3D-array is then considered as argument).…”
Section: Defining and Solving An Integral Equationmentioning
confidence: 99%
“…19 Villamizar and Acosta have continued to develop a variety of curvilinear grids, similar to that used here, and have applied them to scattering from multiple nonconventional objects in two-dimensions. 24,25 III. NUMERICAL SIMULATION The model simulated in this work is scaled down to exactly 1 4 the size of the mathematical model used by Stepanishen and Tougas.…”
Section: Discretizationmentioning
confidence: 99%
“…More precisely following [28], we assume that the obstacle in the upper half-plane is well separated from Γ. Therefore, it can be enclosed by an artificial circular boundary B with radius R, centered at a point b = (b x , b y ) inside the obstacle, which is completely contained in Ω (b y > R).…”
Section: Lemmamentioning
confidence: 99%