• Journal of Applied Optics
  • Vol. 45, Issue 6, 1219 (2024)
Meiqi ZHAO1,2,3, Wei ZHOU1,2,3,*, Di WANG2,3,4,**, Yan LYU1,2,3..., Yushuang LI1,2,3, Yu PU2,3,4, Dong LI2,3,4, Qidong FENG5, Shuxian CHEN5 and Yilang LUO5|Show fewer author(s)
Author Affiliations
  • 1School of Physics and Electronic Engineering, Northeast Petroleum University, Daqing 163318, China
  • 2International Joint Laboratory on Low-Carbon and New-Energy Nexus, Northeast Petroleum University, Daqing 163318, China
  • 3National Key Laboratory of Multi-Resource Collaboration for Green Extraction of Onshore Shale Oil, Daqing 163318, China
  • 4School of Architecture and Civil Engineering, Northeast Petroleum University, Daqing 163318, China
  • 5Hangzhou Hangran Engineering Technology Co.,Ltd., Hangzhou 310008, China
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    DOI: 10.5768/JAO202445.0603002 Cite this Article
    Meiqi ZHAO, Wei ZHOU, Di WANG, Yan LYU, Yushuang LI, Yu PU, Dong LI, Qidong FENG, Shuxian CHEN, Yilang LUO. Optimization analysis of optoelectronic parameters of laser telemetry systems for hydrogen leakage detection in hydrogen-involved equipment[J]. Journal of Applied Optics, 2024, 45(6): 1219 Copy Citation Text show less
    Hydrogen telemetry TDLAS system
    Fig. 1. Hydrogen telemetry TDLAS system
    Light source module
    Fig. 2. Light source module
    Diagram of laser radiation transmission model of non-cooperative target surface
    Fig. 3. Diagram of laser radiation transmission model of non-cooperative target surface
    Module design of open optical path
    Fig. 4. Module design of open optical path
    Data detection module
    Fig. 5. Data detection module
    Output frequency
    Fig. 6. Output frequency
    Centre frequency
    Fig. 7. Centre frequency
    Absorbance ln(I0/It)
    Fig. 8. Absorbance ln(I0/It)
    Detector received light intensity It
    Fig. 9. Detector received light intensity It
    Second harmonic signal
    Fig. 10. Second harmonic signal
    Backward reflected laser power on surface of common non-cooperative targets at different detection distances
    Fig. 11. Backward reflected laser power on surface of common non-cooperative targets at different detection distances
    Relations of light intensity received by detector and F number (changing diameters of pupil)
    Fig. 12. Relations of light intensity received by detector and F number (changing diameters of pupil)
    Relations of light intensity received by detector and F number (changing focal length)
    Fig. 13. Relations of light intensity received by detector and F number (changing focal length)
    Second harmonic signals at different scanning amplitudes
    Fig. 14. Second harmonic signals at different scanning amplitudes
    Second harmonic signals at different scanning frequencies
    Fig. 15. Second harmonic signals at different scanning frequencies
    Optimized laser-echo incident power for different materials at different detection distances
    Fig. 16. Optimized laser-echo incident power for different materials at different detection distances
    Second harmonic signals at different concentrations
    Fig. 17. Second harmonic signals at different concentrations
    表面材料吸收率反射率BRDF
    木板0.0600.94 (A=0.538 6,B=0.8,g=0)
    塑料0.2300.77 (A=0.125 ,B=0.003 5,g=1)
    铝板0.050.948 70.001 3 (A=0.000 1,B=0.015,g=2)
    石灰0.1000.90 (A=0.315 1,B=0.1,g=0)
    Table 1. Parameters of material surface properties
    Meiqi ZHAO, Wei ZHOU, Di WANG, Yan LYU, Yushuang LI, Yu PU, Dong LI, Qidong FENG, Shuxian CHEN, Yilang LUO. Optimization analysis of optoelectronic parameters of laser telemetry systems for hydrogen leakage detection in hydrogen-involved equipment[J]. Journal of Applied Optics, 2024, 45(6): 1219
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