2019
DOI: 10.1016/j.jcp.2019.06.016
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2D elastic plane-wave diffraction by a stress-free wedge of arbitrary angle

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Cited by 5 publications
(4 citation statements)
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References 35 publications
(60 reference statements)
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“…Observing (4.23), we note that at the second members we have that, in general, ψ bs (−m bi (γ , η)) contains discontinuous field components at the boundary u = 0, v < 0 of the angular region, while ψt (η, 0) (by definition 2. 16) is continuous at the boundary u > 0, v = 0. Similarly to what has been done in [1] for electromagnetic applications, we can repeat the procedure to obtain functional equations for regions 3 and 4 (figure 1).…”
Section: (B) From Region 1 To the Other Angular Regionsmentioning
confidence: 99%
See 1 more Smart Citation
“…Observing (4.23), we note that at the second members we have that, in general, ψ bs (−m bi (γ , η)) contains discontinuous field components at the boundary u = 0, v < 0 of the angular region, while ψt (η, 0) (by definition 2. 16) is continuous at the boundary u > 0, v = 0. Similarly to what has been done in [1] for electromagnetic applications, we can repeat the procedure to obtain functional equations for regions 3 and 4 (figure 1).…”
Section: (B) From Region 1 To the Other Angular Regionsmentioning
confidence: 99%
“…An important aspect of this work is the use of recursive equations that provide analytical continuation (propagation of the solution) of the approximate spectral functions obtained by the numerical solution in a certain strip. New developments of this method are reported in [16], where double Fourier transforms are introduced to obtain the kernels of the singular integral equations. In [17], the method is extended to three-dimensional problems, however, the proposed functional equations in spectral domain are again written in terms of singular integral operators and not in an algebraic form.…”
Section: Introductionmentioning
confidence: 99%
“…Note that when doing an asymptotic evaluation of the KA integral on a finite surface, the KA resulting leading terms describe the reflected waves, and the other terms describe diffracted waves by the surface edges which have the same nature (cylindrical or conical wave fronts) but not the same amplitude as those predicted by the geometrical theory of diffraction (GTD) [55,60]. The main advantage of the Kirchhoff approximation is to provide finite results for the scattered field in the whole space, contrary to GTD [61][62][63][64][65]. One of the main inconveniences of the Kirchhoff approximation (KA) is its incorrect quantitative prediction of edges diffraction, since the approximation of the surface field by the geometrical field is invalid near the edges.…”
Section: Theory and Historymentioning
confidence: 99%
“…GTD is preferred to KA for simulating scattering by crack edges (notably for TOFD configurations [8,9]) but fails in the near-incident and specular reflection directions (shadow boundaries). A GTD solution has also recently been proposed for wedge scattering [10][11][12]. Several system models based on KA [3] or GTD [13,14] were conceived first for 2D configurations and then developed in 3D for KA [1,5] and for GTD [15], then using an incremental Huygens model [16].…”
Section: Introductionmentioning
confidence: 99%