• Chinese Journal of Lasers
  • Vol. 47, Issue 12, 1204006 (2020)
Zhang Yueying1, Ni Chenyin1、*, and Shen Zhonghua2
Author Affiliations
  • 1School of Electronic and Optical Engineering, Nanjing University of Science & Technology, Nanjing, Jiangsu 210094, China
  • 2School of Science, Nanjing University of Science & Technology, Nanjing, Jiangsu 210094, China
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    DOI: 10.3788/CJL202047.1204006 Cite this Article Set citation alerts
    Zhang Yueying, Ni Chenyin, Shen Zhonghua. Laser Ultrasonic Monitoring of Reversible/Irreversible Changes in Photo-Thermal Modulation Crack Closure[J]. Chinese Journal of Lasers, 2020, 47(12): 1204006 Copy Citation Text show less
    Schematic of experimental setup
    Fig. 1. Schematic of experimental setup
    Time domain waveforms based on TOFD method in three areas of crack. (a) Start of crack; (b) middle of crack; (c) tip of crack
    Fig. 2. Time domain waveforms based on TOFD method in three areas of crack. (a) Start of crack; (b) middle of crack; (c) tip of crack
    Schematic of sound wave transmission at surface of crack
    Fig. 3. Schematic of sound wave transmission at surface of crack
    Schematic of excitation-detection source scanning path
    Fig. 4. Schematic of excitation-detection source scanning path
    Schematic of location of crack heating area
    Fig. 5. Schematic of location of crack heating area
    Scanning results of tR(heat) peak-peak value when cracks are heated in three photo-thermal cycles. (a) 1st photo-thermal cycle; (b) 2nd photo-thermal cycle; (c) 3rd photo-thermal cycle
    Fig. 6. Scanning results of tR(heat) peak-peak value when cracks are heated in three photo-thermal cycles. (a) 1st photo-thermal cycle; (b) 2nd photo-thermal cycle; (c) 3rd photo-thermal cycle
    Scanning results of tL-R(heat) peak-peak value when cracks are heated in three photo-thermal cycles. (a) 1st photo-thermal cycle; (b) 2nd photo-thermal cycle; (c) 3rd photo-thermal cycle
    Fig. 7. Scanning results of tL-R(heat) peak-peak value when cracks are heated in three photo-thermal cycles. (a) 1st photo-thermal cycle; (b) 2nd photo-thermal cycle; (c) 3rd photo-thermal cycle
    Scanning results of arrival time of tR(heat) signal when crack are heated in first photo-thermal cycle. (a) Area 1; (b) area 2; (c) area 3
    Fig. 8. Scanning results of arrival time of tR(heat) signal when crack are heated in first photo-thermal cycle. (a) Area 1; (b) area 2; (c) area 3
    Curves of average peak-peak value of tR(heat) when cracks are heated. (a) Area 1; (b) area 2; (c) area 3
    Fig. 9. Curves of average peak-peak value of tR(heat) when cracks are heated. (a) Area 1; (b) area 2; (c) area 3
    Curves of average peak-peak value of tL-R(heat) when cracks are heated. (a) Area 1; (b) area 2; (c) area 3
    Fig. 10. Curves of average peak-peak value of tL-R(heat) when cracks are heated. (a) Area 1; (b) area 2; (c) area 3
    Curve of average arrival time of tR(heat) when cracks are heated in first photo-thermal cycle
    Fig. 11. Curve of average arrival time of tR(heat) when cracks are heated in first photo-thermal cycle
    Schematic of surface wave propagation path before crack heating in the first photo-thermal cycle. (a) Area 1; (b) area 2; (c) area 3
    Fig. 12. Schematic of surface wave propagation path before crack heating in the first photo-thermal cycle. (a) Area 1; (b) area 2; (c) area 3
    Zhang Yueying, Ni Chenyin, Shen Zhonghua. Laser Ultrasonic Monitoring of Reversible/Irreversible Changes in Photo-Thermal Modulation Crack Closure[J]. Chinese Journal of Lasers, 2020, 47(12): 1204006
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