2021
DOI: 10.1016/j.jcp.2020.110062
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3D elastic plane-wave diffraction by a stress-free wedge for incident skew angles below the critical angle in diffraction

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Cited by 2 publications
(5 citation statements)
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“…According to the authors' opinion, this technique constitutes a very power tool for the accurate approximate solutions of arbitrary WH equations. We remark that the GWHEs are algebraic, while in [17], the solution is obtained by functional equations written in terms of singular integral operators and solved by numerical technique. We assert that the semianalytic solution using the Fredholm factorization method allows physical insights by asymptotics in spectral domain.…”
Section: Equivalence Theorem In Elasticity: a Field In A Lossy Region Is Uniquely Specified By The Sources Within The Region Plus The Conmentioning
confidence: 99%
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“…According to the authors' opinion, this technique constitutes a very power tool for the accurate approximate solutions of arbitrary WH equations. We remark that the GWHEs are algebraic, while in [17], the solution is obtained by functional equations written in terms of singular integral operators and solved by numerical technique. We assert that the semianalytic solution using the Fredholm factorization method allows physical insights by asymptotics in spectral domain.…”
Section: Equivalence Theorem In Elasticity: a Field In A Lossy Region Is Uniquely Specified By The Sources Within The Region Plus The Conmentioning
confidence: 99%
“…In the following, we assume that the geometry of the elastic wave-motion problem as well as the eventual boundary conditions are invariant along the z-direction, thus, without loss of generality, when a source depends on an ejαo z factor, also the total field depends on the same factor, i.e. bold-italicψt=bold-italicψtfalse(x,y,zfalse)=ffalse(x,yfalse) ejαo z, see for instance [17] before (2.8). Of course, the same behaviour can be obtained by applying a Fourier transform also along the z-direction and assuming an incident plane wave with a particular skew direction that yields ejαo z.…”
Section: First-order Differential Equations For Continuous Components...mentioning
confidence: 99%
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“…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%