2017
DOI: 10.1007/s12046-017-0636-6
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Continuum limit of discrete Sommerfeld problems on square lattice

Abstract: A low frequency approximation of the discrete Sommerfeld diffraction problems, involving the scattering of a time harmonic lattice wave incident on square lattice by a discrete Dirichlet or a discrete Neumann half-plane, is investigated. It is established that the exact solution of the discrete model converges to the solution of the continuum model, i.e. the continuous Sommerfeld problem, in certain discrete Sobolev space defined by W. Hackbusch. The proof of convergence has been provided for both types of bou… Show more

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Cited by 14 publications
(13 citation statements)
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“…Last but not the least, there remains an issue of the continuum limit. For the considered case of positive imaginary part of ω, it is left as an exercise (one possibility involves the tools that are used in [54]) to prove that the low-frequency limit (i.e. with b → 0 but fixed ω and Nb; recall ω = bω) coincides with that of the well-known solution [27,28] provided the separation between the semi-infinite defects N scales naturally as 1/b.…”
Section: Discussionmentioning
confidence: 99%
“…Last but not the least, there remains an issue of the continuum limit. For the considered case of positive imaginary part of ω, it is left as an exercise (one possibility involves the tools that are used in [54]) to prove that the low-frequency limit (i.e. with b → 0 but fixed ω and Nb; recall ω = bω) coincides with that of the well-known solution [27,28] provided the separation between the semi-infinite defects N scales naturally as 1/b.…”
Section: Discussionmentioning
confidence: 99%
“…As the wavelength 2π/k 1 becomes large compared to b, the so called continuum limit is obtained, which can also be perceived as a low frequency approximation in the case of assumed square lattice model. The continuum limit of the discrete Helmholtz equation is the continuous Helmholtz equation [13,43]. From the perspective of the continuum model, the solutions obtained by [4,5] can be seen to be approximated via a lattice formulation and the solution of discrete scattering due to the two staggered cracks.…”
Section: Low Frequency Approximationmentioning
confidence: 99%
“…In the context of the well known solution of the two parallel, staggered plates problem [4,5] in the continuum model, using the numerical solution of the discrete scattering problem, it has been found that, as the frequency approaches zero, the solution coincides with that of the the continuum model, but this is expected [43].…”
Section: Introductionmentioning
confidence: 99%
“…A sketch of the proof of Theorem 4.4 is presented in this paragraph. The detailed statements and rigorous arguments appear in [42], a part of which is already included in the foregoing text; in particular the definitions and statements after (4.13). Suppose that P : H + 1 2 → H + 1 2 (R) is chosen as the suitably defined prolongation operator, which acts in a direction opposite to R .…”
Section: Accepted Manuscriptmentioning
confidence: 99%