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Propagation of laser-generated shock waves in metals: 3D axisymmetric simulations compared to experiments

Article dans une revue avec comité de lecture
Author
CUENCA, Eduardo
505477 Safran Tech
541882 Institut Jean Le Rond d'Alembert [DALEMBERT]
86289 Laboratoire Procédés et Ingénierie en Mécanique et Matériaux [PIMM]
ccDUCOUSSO, Mathieu
505477 Safran Tech
ccRONDEPIERRE, Alexandre
530280 Thales LAS France
86289 Laboratoire Procédés et Ingénierie en Mécanique et Matériaux [PIMM]
ccVIDEAU, Laurent
119523 DAM Île-de-France [DAM/DIF]
1055206 Laboratoire Matière sous Conditions Extrêmes [LMCE]
ccCUVILLIER, Nicolas
505477 Safran Tech
BERTHE, Laurent
86289 Laboratoire Procédés et Ingénierie en Mécanique et Matériaux [PIMM]
ccCOULOUVRAT, François
541882 Institut Jean Le Rond d'Alembert [DALEMBERT]

URI
http://hdl.handle.net/10985/23621
DOI
10.1063/5.0021131
Date
2020-12
Journal
Journal of Applied Physics

Abstract

This work aims at demonstrating the ability of an acoustic linear code to model the propagation of a shock wave created by a laser impact over a metallic surface. In this process, a high pressure surface level is reached using a ns laser pulse that heats the surface of the material and generates a dense plasma expansion. The pressure reaches few GPa so shock waves are generated and propagate into the bulk of the material. Currently, shock wave propagation is modeled using continuity equations and an ad hoc equation of state for the illuminated mate-rial, very limiting because it is numerically intensive. Here, we propose to model the shock wave bulk propagation using a linear acoustic code. A nonlinear surface pressure term, resulting from the laser–matter interaction, is used as a boundary condition. The applied numerical scheme is based on the Virieux scheme, including a fourth order finite difference discretization of the linearized elastomechanical equations. The role of longitudinal and transverse waves and their origins are highlighted. The importance of considering 3D geometries is pointed out. Simulations are finally confronted with experimental results obtained with the Hephaistos Laserlab facility (energy up to 14 J at 532 nm wavelength laser; pulse duration: 7 ns). Illuminations up to the optical breakdown in water are easily achieved with laser focal spots of 5 mm width. Excellent agreement between experiments and simulations is observed for several sets of experimental parameters for titanium, a material of high elastic limit, while limitations are founded for aluminum. The code is available in the MetaData.

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