2015
DOI: 10.1121/1.4922701
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Experimental and numerical study of the excitability of zero group velocity Lamb waves by laser-ultrasound

Abstract: The excitability of zero group velocity (ZGV) Lamb waves using a pulsed laser source is investigated experimentally and through numerical simulation. Experimentally, a laser based ultrasonic technique is used to find the optical spot size on the sample surface that allows an optimal coupling of the optical energy into the ZGV mode. Numerical simulations, using the time domain finite differences technique, are carried out to model the thermoelastic generation process by laser irradiation and the propagation of … Show more

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Cited by 39 publications
(9 citation statements)
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“…The maxima of these curves are in good agreement with theoretical calculations. These results are coherent with the approximation (w ≈ 0.3λ S1S2 ) given for an aluminium plate by Balogun et al 17 Other results were obtained by Grnsteidl et al in a 250-µm thick tungsten plate 19 of Poisson's ratio ν = 0.284 and shear velocity c s = 2668 m/s. With these parameters, the wavelength is λ S1S2 = 3.7 × 2h mm, so that the optimal beam radius to plate thickness ratio is…”
Section: A Optimization Of a Gaussian Beamsupporting
confidence: 89%
See 1 more Smart Citation
“…The maxima of these curves are in good agreement with theoretical calculations. These results are coherent with the approximation (w ≈ 0.3λ S1S2 ) given for an aluminium plate by Balogun et al 17 Other results were obtained by Grnsteidl et al in a 250-µm thick tungsten plate 19 of Poisson's ratio ν = 0.284 and shear velocity c s = 2668 m/s. With these parameters, the wavelength is λ S1S2 = 3.7 × 2h mm, so that the optimal beam radius to plate thickness ratio is…”
Section: A Optimization Of a Gaussian Beamsupporting
confidence: 89%
“…This question was then addressed by Grunsteidl et al experimentally and numerically using a time domain finite difference technique. 19 They found, for tungsten, an optimal radius between 1.0 and 1.1 times the plate thickness.…”
Section: Introductionmentioning
confidence: 97%
“…The filter was necessary as the absorbed energy from the laser heated the surrounding air leading to the variation of the index Δn in the optical path of the probe beam. This induced an additional phase shift Δϕ n and a large low-frequency voltage that would otherwise saturate the electronics detection unit 78 . A video of a typical signal acquisition is provided in Supplementary Movie 1.…”
Section: Methodsmentioning
confidence: 99%
“…The filter was necessary as the absorbed energy from the laser heated the surrounding air leading to the variation of the index ∆n in the optical path of the probe beam. This induced an additional phase shift ∆φ n and a large low frequency voltage that would otherwise saturate the electronics detection unit [45]. A video of a typical signal acquisition FIG.…”
Section: Elastic Guided Waves Measurementsmentioning
confidence: 99%