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<pubDate xmlns="http://apache.org/cocoon/i18n/2.1">Thu, 05 Mar 2026 19:58:24 GMT</pubDate>
<dc:date>2026-03-05T19:58:24Z</dc:date>
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<title>Finite element analysis of laser shock peening of 2050-T8 aluminum alloy</title>
<link>http://hdl.handle.net/10985/9065</link>
<description>Finite element analysis of laser shock peening of 2050-T8 aluminum alloy
HFAIEDH, Neila; PEYRE, Patrice; SONG, Hongbin; POPA, Ioana; JI, Vincent; VIGNAL, Vincent
Laser shock processing is a recently developed surface treatment designed to improve the mechanical properties and fatigue performance of materials, by inducing a deep compressive residual stress field. The purpose of this work is to investigate the residual stress distribution induced by laser shock processing in a 2050-T8 aeronautical aluminium alloy with both X-ray diffraction measurements and 3D finite element simulation. The method of X-ray diffraction is extensively used to characterize the crystallographic texture and the residual stress crystalline materials at different scales (macroscopic, mesoscopic and microscopic). Shock loading and materials’ dynamic response are experimentally analysed using Doppler velocimetry in order to use adequate data for the simulation. Then systematic experience versus simulation comparisons are addressed, considering first a single impact loading, and in a second step the laser shock processing treatment of an extended area, with a specific focus on impact overlap. Experimental and numerical results indicate a residual stress anisotropy, and a better surface stress homogeneity with an increase of impact overlap. A correct agreement is globally shown between experimental and simulated residual stress values, even if simulations provide us with local stress values whereas X-ray diffraction determinations give averaged residual stresses.
</description>
<pubDate>Thu, 01 Jan 2015 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/10985/9065</guid>
<dc:date>2015-01-01T00:00:00Z</dc:date>
<dc:creator>HFAIEDH, Neila</dc:creator>
<dc:creator>PEYRE, Patrice</dc:creator>
<dc:creator>SONG, Hongbin</dc:creator>
<dc:creator>POPA, Ioana</dc:creator>
<dc:creator>JI, Vincent</dc:creator>
<dc:creator>VIGNAL, Vincent</dc:creator>
<dc:description>Laser shock processing is a recently developed surface treatment designed to improve the mechanical properties and fatigue performance of materials, by inducing a deep compressive residual stress field. The purpose of this work is to investigate the residual stress distribution induced by laser shock processing in a 2050-T8 aeronautical aluminium alloy with both X-ray diffraction measurements and 3D finite element simulation. The method of X-ray diffraction is extensively used to characterize the crystallographic texture and the residual stress crystalline materials at different scales (macroscopic, mesoscopic and microscopic). Shock loading and materials’ dynamic response are experimentally analysed using Doppler velocimetry in order to use adequate data for the simulation. Then systematic experience versus simulation comparisons are addressed, considering first a single impact loading, and in a second step the laser shock processing treatment of an extended area, with a specific focus on impact overlap. Experimental and numerical results indicate a residual stress anisotropy, and a better surface stress homogeneity with an increase of impact overlap. A correct agreement is globally shown between experimental and simulated residual stress values, even if simulations provide us with local stress values whereas X-ray diffraction determinations give averaged residual stresses.</dc:description>
</item>
<item>
<title>Residual stresses in surface induction hardening of steels: Comparison between experiment and simulation</title>
<link>http://hdl.handle.net/10985/10519</link>
<description>Residual stresses in surface induction hardening of steels: Comparison between experiment and simulation
COUPARD, Dominique; PALIN-LUC, Thierry; BRISTIEL, Philippe; JI, Vincent; DUMAS, Christian
Deep induction hardening has been performed on two batches of smooth cylindrical specimens with a hardening depth respectively around 2 mm and 3 mm. The distributions of axial and circumferential residual stresses are analysed for the two specimen batches by X-ray diffraction technique. The radial normal stress field is estimated through the use of the well known Moore and Evans correction. Finally, the experimental residual stresses are compared with those obtained from a multiphysic finite element modelling of the whole induction treatment process, including electromagnetic, thermal, metallurgical and mechanical phenomena. The simulated residual stress field is in good agreement with X-ray analysis especially at depths lower than one-tenth the specimen diameter. At deeper depths, a correction of the experimental X-ray analysis has been done to obtain realistic values.
</description>
<pubDate>Tue, 01 Jan 2008 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/10985/10519</guid>
<dc:date>2008-01-01T00:00:00Z</dc:date>
<dc:creator>COUPARD, Dominique</dc:creator>
<dc:creator>PALIN-LUC, Thierry</dc:creator>
<dc:creator>BRISTIEL, Philippe</dc:creator>
<dc:creator>JI, Vincent</dc:creator>
<dc:creator>DUMAS, Christian</dc:creator>
<dc:description>Deep induction hardening has been performed on two batches of smooth cylindrical specimens with a hardening depth respectively around 2 mm and 3 mm. The distributions of axial and circumferential residual stresses are analysed for the two specimen batches by X-ray diffraction technique. The radial normal stress field is estimated through the use of the well known Moore and Evans correction. Finally, the experimental residual stresses are compared with those obtained from a multiphysic finite element modelling of the whole induction treatment process, including electromagnetic, thermal, metallurgical and mechanical phenomena. The simulated residual stress field is in good agreement with X-ray analysis especially at depths lower than one-tenth the specimen diameter. At deeper depths, a correction of the experimental X-ray analysis has been done to obtain realistic values.</dc:description>
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