Laser & Optoelectronics Progress, Volume. 61, Issue 23, 2300005(2024)

Research and Development Prospects of Laser Shock Peening as a Post-Processing Technique for Selective Laser Melting

Xinjie Dai1,2, Jianlei Wang2,3, Yunxia Ye1, Chuanqi Huang2、*, Jiasheng Guo2, Weiqiang Yang4,5, and Yaobin Qu6
Author Affiliations
  • 1School of Mechanical Engineering, Jiangsu University, Zhenjiang 212013, Jiangsu , China
  • 2Intelligent Optoelectronic Detection Center,Nanjing Institute of Advanced Laser Technology, Nanjing 210038, Jiangsu , China
  • 3Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 4College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, Hunan , China
  • 5Nanhu Laser Laboratory, National University of Defense Technology, Changsha 410073, Hunan , China
  • 6Shanghai Institute of Satellite Engineering, Shanghai 201109, China
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    Figures & Tables(11)
    Schematic of LSP principle[12]
    Schematic of RCS and SPD generation[12]
    Residual stress distribution near the hole at laser power densities of 4.7 GW/cm² and 6.6 GW/cm²[14]. (a) Contour map of residual stress distribution; (b) residual stress distribution along the AB line
    Impact of RCS at different overlap ratios. (a) Ref. [16]; (b) Ref. [17]
    Impact test results[19]. (a) Average grain size of each sample; (b) cross-sectional microhardness distribution curves for each sample
    Cross-sectional grain morphology of the original sample[21]. (a) Semi-circular melt pool boundary; (b) refined morphology in the blue dashed-line region; (c) pores
    Cross-sectional grain morphology of LSP-ed sample[21]. (a) Deformed layer; (b) refined microstructure within the blue dashed-line frame; (c) microhardness of the original and LSP-ed samples
    Fatigue crack initiation and fatigue crack growth in LSP-treated Ti6Al4V titanium alloy[30]. (a) Crack length variation with cycle numbers at different laser shock intensities; (b)values of C and m for different sets of materials derived from the Paris equation fitting; (c)‒(f) functional relationship between FCG rate and crack length, as well as the relationship between FCG rate and ΔK; (g) (h) enlarged images of localized regions
    S-N curves of LSP and HT [33]
    Influence of different processing methods on sample cracks[33]. (a) Macroscopic appearance of the fracture surface of high-temperature specimens; (b) unmelted powder with stress of 400 MPa and 8.29×104 cycles; (c) regions exhibiting incomplete fusion with stress of 340 MPa and 2.78×105 cycles; (d) clusters of α-phase with stress of 280 MPa and 5.52×108 cycles; (e) stress of 370 MPa and 3.57×107 cycles
    Comparative charts before and after using LSPwC[43]. (a) Sa; (c) Ra; (b)(d) surface roughness profile
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    Xinjie Dai, Jianlei Wang, Yunxia Ye, Chuanqi Huang, Jiasheng Guo, Weiqiang Yang, Yaobin Qu. Research and Development Prospects of Laser Shock Peening as a Post-Processing Technique for Selective Laser Melting[J]. Laser & Optoelectronics Progress, 2024, 61(23): 2300005

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    Paper Information

    Category: Reviews

    Received: Feb. 5, 2024

    Accepted: Apr. 14, 2024

    Published Online: Nov. 26, 2024

    The Author Email: Chuanqi Huang (hcq960512@163.com)

    DOI:10.3788/LOP240663

    CSTR:32186.14.LOP240663

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