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1. 2. 3. © Laser-Shock Processing Of Steel Yibas, BS; Shuja, SZ; Arif, A; Gondal, MA ELSEVIER SCIENCE SA, JOURNAL OF MATERIALS PROCESSING TECHNOLOGY; pp:

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Presentation on theme: "1. 2. 3. © Laser-Shock Processing Of Steel Yibas, BS; Shuja, SZ; Arif, A; Gondal, MA ELSEVIER SCIENCE SA, JOURNAL OF MATERIALS PROCESSING TECHNOLOGY; pp:"— Presentation transcript:

1 1. 2. 3. © Laser-Shock Processing Of Steel Yibas, BS; Shuja, SZ; Arif, A; Gondal, MA ELSEVIER SCIENCE SA, JOURNAL OF MATERIALS PROCESSING TECHNOLOGY; pp: 6-17; Vol: 135 King Fahd University of Petroleum & Minerals http://www.kfupm.edu.sa Summary The laser induced shock hardening of metal surfaces has several advantages over the conventional surface hardening methods. In order to improve the shock hardening process, investigation into the physical processes involved is necessary. In the present study, the modeling of the laser pulsed heating process is considered and the closed form solution for the surface temperature rise is obtained. The recoil pressure developed during the surface ablation is formulated and the elastic-plastic wave generation due to impact loading of the surface is analyzed. The surface temperature profile, the magnitude of the recoil pressure, and the depth of resulting plastic region inside the substrate are predicted for mild and stainless steel workpieces. The study is extended to include experimental investigation of laser-shock processing. Nd:YAG laser is used to ablate the steel surfaces. SEM, TEM, and EDS are carried out for metallurgical and morphological examinations of the laser ablated region. Microhardness measurement is carried out and the prediction of depth of plastic zone from the wave propagation analysis is validated. It is found that the recoil pressure in the order of I GPa is developed at the surface. The dislocations are generated in the surface vicinity of the substrate after the laser ablation of the surface due to the impact loading of the surface by a recoil pressure. The plastic zone extends about 450 mum below the surface and the predictions well agreed with the experimental findings. (C) 2002 Elsevier Science B.V. All rights reserved. References: CHU JP, 1999, MAT SCI ENG A-STRUCT, V260, P260 CLAUER AH, 1981, SHOCK WAVES HIGH STR, P675 DEVAUX D, 1993, J APPL PHYS, V74, P2268 Copyright: King Fahd University of Petroleum & Minerals; http://www.kfupm.edu.sa

2 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. 17. 18. 19. 20. © FABBRO R, 1993, J APPL PHYS, V68, P2268 FREITAS M, 1993, MAT SCI ENG A-STRUCT, V167, P115 GERLAND M, 1992, MAT SCI ENG A-STRUCT, V156, P175 GUDONOV SK, 1959, MAT SBORNIK, P271 KAR A, 1995, OPT QUANT ELECTRON, V27, P1165 PEYRE P, 1995, OPT QUANT ELECTRON, V27, P1213 PEYRE P, 1996, J LASER APPL, V8, P135 ROMAIN JP, 1988, SHOCK WAVES CONDENSE, P787 SEMAK V, 1997, J PHYS D APPL PHYS, V30, P2541 XIAO L, 1996, NUMERICAL COMPUTATIO YILBAS BS, 1988, PRAMANA-J PHYS, V31, P365 YILBAS BS, 1990, PRAMANA-J PHYS, V34, P473 YILBAS BS, 1992, PRAMANA-J PHYS, V38, P195 YILBAS BS, 1995, INT J MACH TOOL MANU, V35, P1047 YILBAS BS, 1997, MATER MANUF PROCESS, V12, P1163 YILBAS BS, 1998, INT J HEAT MASS TRAN, V41, P1969 YILBAS BS, 1998, P I MECH ENG C-J MEC, V212, P141 For pre-prints please write to: magondal@kfupm.edu.sa Copyright: King Fahd University of Petroleum & Minerals; http://www.kfupm.edu.sa


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