1989
DOI: 10.1063/1.342956
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Transient generation by a wide thermoelastic source at a solid surface

Abstract: A method for computing the radiation from a thermal expansion source, generated at a solid surface by a laser pulse of finite width, is evaluated for two radial beam energy distributions. A theoretical expression for the impulse response is obtained for two components of the displacement at any point within the solid, and may be used to compute the field for an arbitrary time excitation. Numerical results are presented, and are compared to experimental results for generation by a pulsed laser.

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Cited by 35 publications
(22 citation statements)
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“…In some experiments, the specific time profile ofthe epicentral displacement generated by laser irradiation of a constraining layer consisting of a transparent material placed over the irradiated face of the target 17 has been clearly exhibited, but the analytical relation between the propagation of the longitudinal waves and the normal displacement at the epicenter has not been determined except for transparent layer having the same elastic and thermal properties that the metallic substrate 18,19 The normal displacement at the epicentre (Fig. 2a) was recorded for a metallic substrate and for a transparent coating on a metallic substrate using the contactless experimental arrangement of Fig.…”
Section: Methodsmentioning
confidence: 99%
“…In some experiments, the specific time profile ofthe epicentral displacement generated by laser irradiation of a constraining layer consisting of a transparent material placed over the irradiated face of the target 17 has been clearly exhibited, but the analytical relation between the propagation of the longitudinal waves and the normal displacement at the epicenter has not been determined except for transparent layer having the same elastic and thermal properties that the metallic substrate 18,19 The normal displacement at the epicentre (Fig. 2a) was recorded for a metallic substrate and for a transparent coating on a metallic substrate using the contactless experimental arrangement of Fig.…”
Section: Methodsmentioning
confidence: 99%
“…Assuming the Lorentz force is decomposed spatially into N force components, the total displacement for these temporal delta force components is given by, where ⊗ denotes a convolution operation, ( ) f t is the temporal dependence of Lorentz force, ( , , 0, ) u t x y z δ = is the total displacement for these temporal delta force components of each circular source (piston or ring source), and is given by, with temporal dependence of delta function [11][12] . In same way, the solution to line coil can be deduced, but will not be given here due to limit space.…”
Section: Methodsmentioning
confidence: 99%
“…Due to the complexity of the problem, an analytical solution is only available for some simple uniform force distributions, such as uniform normal piston force and uniform radially acting ring force [1,3,[11][12] . Accordingly, transient field studies were carried out generally by the Finite Element Method (FEM) [7][8][9] .…”
Section: Introductionmentioning
confidence: 99%
“…34 In some experiments, the specific time profile of the epicentral displacement generated by laser irradiation of a constraining layer consisting of a transparent material placed over the irradiated face of the target, 35 or a polymer coating, 22 has been clearly exhibited, but the relation between the propagation of the waves and the normal displacement at the epicenter has not been determined except for transparent layers having the same elastic and thermal properties as the metallic substrate. 36,37 The aim of the present study is to propose an alternative method using laser ultrasonics devoted to assess the practical adhesion of transparent coatings. Subsequently, acoustic modeling is performed and this leads to the integrity interface characterization.…”
Section: Introductionmentioning
confidence: 99%