2014
DOI: 10.1093/imamat/hxu023
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Non-principal Rayleigh waves in deformed transversely isotropic incompressible non-linearly elastic solids

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Cited by 14 publications
(7 citation statements)
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“…In passing, we note that our formulation particularized for transversely isotropic materials and isotropic materials coincides with the ones given in [62] and [84], respectively. In particular, for instance, the matrices N 1 , N 2 and K in (3.21) particularized for isotropic materials coincide, respectively, with the matrices N 1 , N 2 and N 3 + XI, where X = ρc 2 , given by (2.9) and (2.10) in [84].…”
Section: The Stroh Formulationmentioning
confidence: 71%
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“…In passing, we note that our formulation particularized for transversely isotropic materials and isotropic materials coincides with the ones given in [62] and [84], respectively. In particular, for instance, the matrices N 1 , N 2 and K in (3.21) particularized for isotropic materials coincide, respectively, with the matrices N 1 , N 2 and N 3 + XI, where X = ρc 2 , given by (2.9) and (2.10) in [84].…”
Section: The Stroh Formulationmentioning
confidence: 71%
“…In chapter three, we extend the analysis presented in chapter 2 [62] dealing with Rayleigh waves for materials reinforced with one family of fibers to obtain the explicit and implicit secular equations of non-principal Rayleigh waves propagating in imcompressible materials reinforced with two families of fibers in the framework of nonlinear elasticity [63].…”
Section: Acknowledgementmentioning
confidence: 99%
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