• Laser & Optoelectronics Progress
  • Vol. 55, Issue 12, 121409 (2018)
Cheng Tao1、2、**, Anmin Yin1、2、*, Zhiqi Ying1, Yufan Wang1、2, Xuedao Shu1、2, and Wenfei Peng1、2
Author Affiliations
  • 1 Faculty of Mechanical Engineering & Mechanics, Ningbo University, Ningbo, Zhejiang 315211, China;
  • 2 Key Laboratory of Roll Forming Technology of Zhejiang Province, Ningbo, Zhejiang 315211, China
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    DOI: 10.3788/LOP55.121409 Cite this Article Set citation alerts
    Cheng Tao, Anmin Yin, Zhiqi Ying, Yufan Wang, Xuedao Shu, Wenfei Peng. Quantitative Analysis of Surface-Breaking Defects by Surface Acoustic Waves Under Different Temperatures[J]. Laser & Optoelectronics Progress, 2018, 55(12): 121409 Copy Citation Text show less
    Schematic of numerical model
    Fig. 1. Schematic of numerical model
    Schematic of mesh generation
    Fig. 2. Schematic of mesh generation
    Schematic of surface defect detection by SLS
    Fig. 3. Schematic of surface defect detection by SLS
    Displacement signals at upper surface by laser source irradiation for different distances from detection point. (a) 1 mm; (b) 1.2 mm; (c) 1.4 mm; (d) 1.7 mm; (e) 2.4 mm
    Fig. 4. Displacement signals at upper surface by laser source irradiation for different distances from detection point. (a) 1 mm; (b) 1.2 mm; (c) 1.4 mm; (d) 1.7 mm; (e) 2.4 mm
    Displacement signals of laser-induced surface acoustic waves under different temperatures. (a) No defects; (b) with defects
    Fig. 5. Displacement signals of laser-induced surface acoustic waves under different temperatures. (a) No defects; (b) with defects
    Waveforms in frequency domain of laser-induced surface acoustic waves under different temperatures
    Fig. 6. Waveforms in frequency domain of laser-induced surface acoustic waves under different temperatures
    Displacement waveforms at different defect depths
    Fig. 7. Displacement waveforms at different defect depths
    Time difference δtAB versus defect depth under different temperatures
    Fig. 8. Time difference δtAB versus defect depth under different temperatures
    Displacement waveforms at different defect widths
    Fig. 9. Displacement waveforms at different defect widths
    Time difference δtAB versus defect width under different temperatures
    Fig. 10. Time difference δtAB versus defect width under different temperatures
    Finite element model of interaction between surface acoustic wave and front edge of defects
    Fig. 11. Finite element model of interaction between surface acoustic wave and front edge of defects
    Displacement fields of front edge of defects interacting with surface acoustic wave. (a) t=0.3 μs; (b) t=0.5 μs; (c) t=0.6 μs
    Fig. 12. Displacement fields of front edge of defects interacting with surface acoustic wave. (a) t=0.3 μs; (b) t=0.5 μs; (c) t=0.6 μs
    Propagation path produced by front edge of defects interacting with surface acoustic wave
    Fig. 13. Propagation path produced by front edge of defects interacting with surface acoustic wave
    Signal in time domain of front edge of defects interacting with surface acoustic wave
    Fig. 14. Signal in time domain of front edge of defects interacting with surface acoustic wave
    Finite element model of interaction between surface acoustic wave and rear edge of defects
    Fig. 15. Finite element model of interaction between surface acoustic wave and rear edge of defects
    Displacement signal of surface acoustic wave interacting with rear edge of defects
    Fig. 16. Displacement signal of surface acoustic wave interacting with rear edge of defects
    Displacement fields of rear edge of defects interacting with surface acoustic wave. (a) t=0.3 μs; (b) t=0.4 μs; (c) t=0.6 μs; (d) t=0.7 μs
    Fig. 17. Displacement fields of rear edge of defects interacting with surface acoustic wave. (a) t=0.3 μs; (b) t=0.4 μs; (c) t=0.6 μs; (d) t=0.7 μs
    Schematic of propagation of feature point K
    Fig. 18. Schematic of propagation of feature point K
    Schematic of interaction process between surface acoustic wave and surface defects
    Fig. 19. Schematic of interaction process between surface acoustic wave and surface defects
    ParameterAbsorptivityDensity /(kg·m-3)Specific heat /(J·kg-1·K-1)Thermalconductivecoefficient /(W·m-1·K-1)Youngmodulus /GPaPoissonratioThermalexpansioncoefficient /(10-5·K-1)
    Expression0.052+3×10-5(T-300)249.5-0.08T780.3+0.48T2769-0.22T85-0.05T0.34+10-4×(T-300)17.7+0.018T
    Table 1. Thermophysical and mechanical parameters of aluminum used for calculation
    Depth /mmtK /μstL /μs
    Numerical resultTheoretical resultNumerical resultTheoretical result
    0.151.2251.2071.3211.310
    0.201.2551.2411.3921.379
    0.251.2861.2761.4551.448
    0.301.3121.3101.5211.517
    Table 2. Numerical and theoretical results of arrival time of feature points K and L
    Depth /mmT=300 KT=500 KT=700 K
    D' /mmRelative error /%D' /mmRelative error /%D' /mmRelative error /%
    0.100.123223.200.120820.800.120020.00
    0.150.175516.970.167811.870.173215.47
    0.200.224812.380.220110.090.21276.35
    0.250.26686.720.26184.720.25722.88
    0.300.31123.730.30882.930.30692.30
    0.350.36542.710.35581.660.35290.83
    Table 3. Relative errors between numerical and theoretical results of defect depth
    Cheng Tao, Anmin Yin, Zhiqi Ying, Yufan Wang, Xuedao Shu, Wenfei Peng. Quantitative Analysis of Surface-Breaking Defects by Surface Acoustic Waves Under Different Temperatures[J]. Laser & Optoelectronics Progress, 2018, 55(12): 121409
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