Laser Simulation of Hypervelocity Impact into Porous Graphite

Abstract Introduction The use of laser-driven shocks is a very interesting alternative to extend the range of impacts accessible by launchers. When a high-power laser is focused on an absorbing target, the first few micrometers of matter vaporizes. The resulting plasma expands violently and pushes against the target surface as shown in Figure 1. By choosing the right laser parameters, the pressure field generated on the target surface can be equivalent to the pressure field that would have been generated by a real projectile.

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Published
2024-09-13
DOI
https://doi.org/10.1115/hvis2024-033
Citations
1
Primary Topic
High-Velocity Impact and Material Behavior
Type
article
Field-Weighted Citation Impact
0.12

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Laser Simulation of Hypervelocity Impact into Porous Graphite

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1 citations
High-Velocity Impact and Material Behavior
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Laser Simulation of Hypervelocity Impact into Porous Graphite

L. Videau, E. Lescoute, David G. Hebert, Laurent Berthe, Bertrand Aubert, Jean‐Luc Rullier
article en
1 citations

Abstract

Abstract Introduction The use of laser-driven shocks is a very interesting alternative to extend the range of impacts accessible by launchers. When a high-power laser is focused on an absorbing target, the first few micrometers of matter vaporizes. The resulting plasma expands violently and pushes against the target surface as shown in Figure 1. By choosing the right laser parameters, the pressure field generated on the target surface can be equivalent to the pressure field that would have been generated by a real projectile.

CEA CESTA (FR), Centre National de la Recherche Scientifique (FR), Arts et Métiers (FR), Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR), CEA DAM Île-de-France (FR), Laboratoire Procédés et Ingénierie en Mécanique et Matériaux (FR)
Centre National de la Recherche Scientifique, Japan Aerospace Exploration Agency
Affordable and clean energy
Openalex Percentile: Top 56%
High-Velocity Impact and Material Behavior
0.12
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