2006
DOI: 10.1007/s10659-005-9023-3
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Partial Uniqueness and Obstruction to Uniqueness in Inverse Problems for Anisotropic Elastic Media

Abstract: We consider the inverse problem of identifying the density and elastic moduli for threedimensional anisotropic elastic bodies, given displacement and traction measurements made at their surface. These surface measurements are modelled by the dynamic Dirichlet-to-Neumann map on a finite time interval. For linear or nonlinear anisotropic hyperelastic bodies we show that the displacement-to-traction surface measurements do not change when the density and elasticity tensor in the interior are transformed tensorial… Show more

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Cited by 26 publications
(29 citation statements)
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References 35 publications
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“…The above results generalize and extend those of Mazzucato & Rachele (2006) for finite hyperelasticity. Our approach, however, uses only elementary methods, and does not require lengthy calculations in local coordinates.…”
Section: Particle Relabelling Transformationssupporting
confidence: 83%
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“…The above results generalize and extend those of Mazzucato & Rachele (2006) for finite hyperelasticity. Our approach, however, uses only elementary methods, and does not require lengthy calculations in local coordinates.…”
Section: Particle Relabelling Transformationssupporting
confidence: 83%
“…Pendry et al 2006;Rahm et al 2008). Of particular relevance to geophysics is the work of Mazzucato & Rachele (2006), who establish non-uniqueness results for both finite and linearized elasticity. Though the situation considered by these authors (the so-called Dirichlet-to-Neumann map) is not directly relevant to surface observations in seismology, it is clear that their methods could be extended in a suitable manner.…”
Section: Downloaded Frommentioning
confidence: 99%
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“…Geometric linearization of elasticity was first introduced by Marsden and Hughes [29] and was further developed by Yavari and Ozakin [43]. See also [33] for similar discussions. Here, we start with a temperature-dependent material manifold and its motion in an ambient space.…”
Section: Linearized Theory Of Thermal Stressesmentioning
confidence: 99%
“…Proof of Equation (17). It follows, for example, from the proof of [25,Lemma 2.7], that the determinant of the principal symbol of P ρ,C is given by (−ρτ 2 + α)…”
Section: Proofsmentioning
confidence: 99%