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1996
DOI: 10.1016/0921-5093(95)10084-9
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Laser shock processing of aluminium alloys. Application to high cycle fatigue behaviour

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Cited by 640 publications
(363 citation statements)
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“…To simplify the model, the function is assumed to be linear according to the hardness and residual stress distribution tests across the peened layer section of former studies [10,11]. By measuring the microhardness across the cross-section of the GHL, Peyre et al [10] found that the hardnesses decreases almost linearly along the depth and finally reach a level identical to the base material. The impact toughness is highest at the surface of the specimen and decreases linearly along the GHL.…”
Section: Modeling Of the Impact Toughness Of A Gradient Hardened Layermentioning
confidence: 99%
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“…To simplify the model, the function is assumed to be linear according to the hardness and residual stress distribution tests across the peened layer section of former studies [10,11]. By measuring the microhardness across the cross-section of the GHL, Peyre et al [10] found that the hardnesses decreases almost linearly along the depth and finally reach a level identical to the base material. The impact toughness is highest at the surface of the specimen and decreases linearly along the GHL.…”
Section: Modeling Of the Impact Toughness Of A Gradient Hardened Layermentioning
confidence: 99%
“…It was reported by Mats et al [9] that the increase of the impact toughness for the steel 15Kh2NMFA upon high-temperature ultrasonic treatment of various durations is due to the formation of a uniform defect structure. For the LSP processing technology, the mechanical properties of the hardened layer are not uniform [1,2,[10][11][12]. By the micro-hardness tests across the LSP peened layer, Peyre et al [10] reported that the hardness decreases gradually from surface to the base material.…”
Section: Introductionmentioning
confidence: 99%
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“…LSP is based on the application of a high intensity pulsed laser beam (Instant peak power density, I > 1 GW/cm 2 ; Laser pulse characteristic duration, τ < 50 ns) at the interface between the metallic target and the surrounding medium (a transparent confining material, normally water) forcing a sudden vaporization of the metallic surface into a high temperature and density plasma that immediately develops inducing a shock wave propagating into the material [2]. This shock wave induces plastic deformation and a residual stress distribution in the target material (if its peak pressure is greater than the dynamic yield limit) able to protect the component by means of a compressive residual stresses (RSs) field.…”
Section: Problem Definition and Theoretical/experimental Methodologymentioning
confidence: 99%
“…The capability of Laser Shock Processing (LSP) for the induction of residual stress fields in sub-surface layers of relatively thick specimens (d > 6 mm) in view of the improvement of their fatigue life has been widely demonstrated [1][2][3][4]. However, the LSP treatment of relatively thin specimens (normally d < 6 mm, but also thicker ones depending on the treatment intensity) brings, as an additional consequence, the possible bending of the treated specimen, a feature that can otherwise be employed for forming procedures according to the laser shock forming process.…”
Section: Introductionmentioning
confidence: 99%