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https://doi.org/10.1016/j.procir.2020.02.062
DC Field | Value | |
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dc.title | Laser peening of 420 martensitic stainless steel using ultrashort laser pulses | |
dc.contributor.author | Maharjan, N. | |
dc.contributor.author | Lin, Z. | |
dc.contributor.author | Ardi, D.T. | |
dc.contributor.author | Ji, L. | |
dc.contributor.author | Hong, M. | |
dc.date.accessioned | 2021-08-10T03:06:57Z | |
dc.date.available | 2021-08-10T03:06:57Z | |
dc.date.issued | 2020 | |
dc.identifier.citation | Maharjan, N., Lin, Z., Ardi, D.T., Ji, L., Hong, M. (2020). Laser peening of 420 martensitic stainless steel using ultrashort laser pulses. Procedia CIRP 87 : 279-284. ScholarBank@NUS Repository. https://doi.org/10.1016/j.procir.2020.02.062 | |
dc.identifier.issn | 2212-8271 | |
dc.identifier.uri | https://scholarbank.nus.edu.sg/handle/10635/196238 | |
dc.description.abstract | Laser shock peening is an established method used to increase resistance of a surface to cracking and fatigue damage by inducing deep compressive residual stresses. Most of the current laser shock peening system utilizes a nanosecond pulse laser with very slow repetition rate (about 5-10 Hz), high pulse energy and a confining medium to constrain the plasma. On the other hand, ultrashort pulse lasers generally have a higher peak power density and operate at higher repetition rate than nanosecond pulse laser. Therefore, there is an opportunity to employ ultrashort pulse lasers to peen the surface in a fast and efficient way. However, limited studies have been performed to investigate the peening capability of ultrashort laser pulses. In this study, femtosecond (fs) pulse laser is used to peen a 420 martensitic steel surface under different coverage. The results show that fs laser can induce peening effect; however, peened depths are much smaller (around 20-30 ?m) compared to high energy nanosecond pulse laser peening (up to 1 mm). A maximum compressive stresses of about -80 MPa was recorded at 981% coverage. Increase in coverage produced stress relaxation and did not increase the depth of influence. It was found that the state of the residual stresses depends on four main factors - intensity of ablation-induced shock wave, thermal effect of laser beam, phase transformation of the steel and surface mechanisms such as presence of nano-ripples and oxidation. Further experiments are ongoing to achieve higher magnitude of compressive residual stresses and higher depth of influence. © 2020 The Author(s). | |
dc.publisher | Elsevier B.V. | |
dc.rights | Attribution-NonCommercial-NoDerivatives 4.0 International | |
dc.rights.uri | http://creativecommons.org/licenses/by-nc-nd/4.0/ | |
dc.source | Scopus OA2020 | |
dc.subject | femtosecond pulse laser | |
dc.subject | hardness | |
dc.subject | laser shock peening | |
dc.subject | residual stresses | |
dc.type | Conference Paper | |
dc.contributor.department | ELECTRICAL AND COMPUTER ENGINEERING | |
dc.description.doi | 10.1016/j.procir.2020.02.062 | |
dc.description.sourcetitle | Procedia CIRP | |
dc.description.volume | 87 | |
dc.description.page | 279-284 | |
Appears in Collections: | Elements Staff Publications |
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