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J. Kollman, A. Merdes, L. Mourey, D. Agard (2011)
Microtubule nucleation by γ-tubulin complexesNature Reviews Molecular Cell Biology, 12
S.P. Lyon, J.D. Johnson
SESAME: The Los Alamos National Laboratory equation of state database
M. Furió, J. González, C. Álvarez, M. Bolaños, J. Moreno (2010)
Analysis of plasma thermal surface effects on the residual stress field induced by LSP in Al2024-t351
J. Macfarlane, I. Golovkin, P. Woodruff (2006)
HELIOS-CR – A 1-D radiation-magnetohydrodynamics code with inline atomic kinetics modelingJournal of Quantitative Spectroscopy & Radiative Transfer, 99
M. Morales, J. Ocaña, C. Molpeceres, J. Porro, Á. García-Beltrán (2008)
Model based optimization criteria for the generation of deep compressive residual stress fields in high elastic limit metallic alloys by ns-laser shock processingSurface & Coatings Technology, 202
J. Ocaña, M. Morales, C. Molpeceres, J. Torres (2004)
Numerical simulation of surface deformation and residual stresses fields in laser shock processing experimentsApplied Surface Science, 238
R. Fabbro, J. Fournier, P. Ballard, D. Devaux, J. Virmont (1990)
Physical study of laser-produced plasma in confined geometryJournal of Applied Physics, 68
G.R. Johnson, W.H. Cook
A constitutive model and data for metals subjected to large strains, high strain rates and high temperatures
J.L. Ocaña
A review on the physics and calculational methods for the modelling of the laser‐matter interaction in high intensity laser processing applications
M. Furió, J. Moreno, C. Álvarez, J. González, Á. Beltrán (2008)
Model based optimization criteria for the generation of deep compressive residual stress fields in high elastic limit metallic alloys by ns-laser shock processing
R. Griffin, B. Justus, A. Campillo, L. Goldberg (1986)
Interferometric studies of the pressure of a confined laser‐heated plasmaJournal of Applied Physics, 59
J. Ocaña, C. Molpeceres, J. Porro, G. Gomez, M. Morales (2004)
Experimental assessment of the influence of irradiation parameters on surface deformation and residual stresses in laser shock processed metallic alloysApplied Surface Science, 238
P. Peyre, X. Scherpereel, L. Berthe, R. Fabbro (1998)
Current trends in laser shock processingSurface Engineering, 14
ABAQUS
ABAQUS User's Manual
A. Clauer, J. Holbrook, B. Fairand (1981)
Effects of Laser Induced Shock Waves on Metals
Y. Sano, N. Mukai, K. Okazaki, M. Obata (1997)
Residual stress improvement in metal surface by underwater laser irradiationNuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms, 121
G. Kay
Failure modeling of titanium 6Al‐4V and aluminum 2024‐T3 with the Johnson‐Cook material model
M. Morales, J. Porro, C. Molpeceres, M. Holgado, J. Ocaña (2010)
Analysis of plasma thermal surface effects on the residual stress field induced by LSP in A12024-t351Journal of Optoelectronics and Advanced Materials, 12
M. Morales, J. Porro, M. Blasco, C. Molpeceres, J. Ocaña (2009)
Numerical simulation of plasma dynamics in laser shock processing experimentsApplied Surface Science, 255
Purpose – Laser shock peening (LSP) is mainly a mechanical process, but in some cases, it is performed without a protective coating and thermal effects are present near the surface. The numerical study of thermo‐mechanical effects and process parameter influence in realistic conditions can be used to better understand the process. Design/methodology/approach – A physically comprehensive numerical model (SHOCKLAS) has been developed to systematically study LSP processes with or without coatings starting from laser‐plasma interaction and coupled thermo‐mechanical target behavior. Several typical results of the developed SHOCKLAS numerical system are presented. In particular, the application of the model to the realistic simulation (full 3D dependence, non‐linear material behavior, thermal and mechanical effects, treatment over extended surfaces) of LSP treatments in the experimental conditions of the irradiation facility used by the authors is presented. Findings – Target clamping has some influence on the results and needs to be properly simulated. An increase in laser spot radius and an increase in pressure produces an increase of the maximum compressive residual stress and also the depth of the compressive residual stress region. By increasing the pulse overlapping density, no major improvements are obtained if the pressure is high enough. The relative influence of thermal/mechanical effects shows that each effect has a different temporal scale and thermal effects are limited to a small region near the surface and compressive residual stresses very close to the surface level can be induced even without any protective coating through the application of adjacent pulses. Originality/value – The paper presents numerical thermo‐mechanical study for LSP treatments without coating and a study of the influence of several process parameters on residual stress distribution with consideration of pulse overlapping.
International Journal of Structural Integrity – Emerald Publishing
Published: Mar 8, 2011
Keywords: Stress (materials); Simulation
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