• Chinese Journal of Lasers
  • Vol. 46, Issue 7, 0701008 (2019)
Wei Wang1、*, Yiguang Yang1, Weihong Zhang1, Xujin Li1, and Degang Xu2
Author Affiliations
  • 1 Pilot National Laboratory for Marine Science and Technology, Qingdao, Shandong 266200, China
  • 2 Tianjin University, school of Precision Instruments & Opto-Electronics Engineering, Tianjin 300072, China;
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    DOI: 10.3788/CJL201946.0701008 Cite this Article Set citation alerts
    Wei Wang, Yiguang Yang, Weihong Zhang, Xujin Li, Degang Xu. Pulsed-Laser-Sound-Signal Detection Based on Frequency-Domain Energy Detector[J]. Chinese Journal of Lasers, 2019, 46(7): 0701008 Copy Citation Text show less
    Experimental setup diagram of generation and collection of laser acoustic signal
    Fig. 1. Experimental setup diagram of generation and collection of laser acoustic signal
    Time-domain and frequency-domain waveforms under different spot diameters. (a) Time-domain waveform; (b) frequency-domain waveform
    Fig. 2. Time-domain and frequency-domain waveforms under different spot diameters. (a) Time-domain waveform; (b) frequency-domain waveform
    Time-domain and frequency-domain waveforms under different laser pulse widths. (a) Time-domain waveform; (b) frequency-domain waveform
    Fig. 3. Time-domain and frequency-domain waveforms under different laser pulse widths. (a) Time-domain waveform; (b) frequency-domain waveform
    Time-domain waveform and power spectrum of laser-sound at different time. (a) Time-domain waveform; (b) power spectrum
    Fig. 4. Time-domain waveform and power spectrum of laser-sound at different time. (a) Time-domain waveform; (b) power spectrum
    Power spectrum of laser-sound signal with different laser energies
    Fig. 5. Power spectrum of laser-sound signal with different laser energies
    Absorptivity in underwater acoustic channel at different frequencies
    Fig. 6. Absorptivity in underwater acoustic channel at different frequencies
    Simulation results of laser-sound signal under sound velocity gradient generated by HM2000 0370 ARGO buoy. (a) Sound velocity gradient generated by HM2000 0370 ARGO buoy; (b) three-dimensional propagation loss of laser-sound signal
    Fig. 7. Simulation results of laser-sound signal under sound velocity gradient generated by HM2000 0370 ARGO buoy. (a) Sound velocity gradient generated by HM2000 0370 ARGO buoy; (b) three-dimensional propagation loss of laser-sound signal
    Power spectrum of laser-sound signals at different distances
    Fig. 8. Power spectrum of laser-sound signals at different distances
    Pre-compensation energy detector
    Fig. 9. Pre-compensation energy detector
    Monte-Carlo simulation process of pre- compensation energy detector
    Fig. 10. Monte-Carlo simulation process of pre- compensation energy detector
    Monte-Carlo simulation result of pre- compensation energy detector
    Fig. 11. Monte-Carlo simulation result of pre- compensation energy detector
    Time-domain signal and power spectrum in tank test. (a) Time-domain signal; (b) power spectrum
    Fig. 12. Time-domain signal and power spectrum in tank test. (a) Time-domain signal; (b) power spectrum
    No. of frequency bandPower percentage /%
    901 ms1901 ms2901 ms
    Frequency band 1 (0-50 kHz)12.2612.0211.96
    Frequency band 2 (50-100 kHz)77.0173.5373.02
    Frequency band 3 (100-150 kHz)9.7913.2913.61
    Total power percentage99.0698.8498.59
    Table 1. Statistical results of signal power under different time
    No. of frequency bandPower percentage /%
    50 mJ100 mJ120 mJ180 mJ320 mJ
    Frequency band 1 (0-50 kHz)10.4110.6810.428.858.44
    Frequency band 2 (50-100 kHz)85.0684.9785.2987.1786.69
    Frequency band 3 (100-150 kHz)4.293.923.973.704.62
    Total power percentage99.7699.5799.6899.7299.75
    Table 2. Statistical results of laser-sound signal power with different laser powers
    Wei Wang, Yiguang Yang, Weihong Zhang, Xujin Li, Degang Xu. Pulsed-Laser-Sound-Signal Detection Based on Frequency-Domain Energy Detector[J]. Chinese Journal of Lasers, 2019, 46(7): 0701008
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