Chinese Journal of Lasers, Volume. 50, Issue 14, 1410002(2023)

Determination of Boundary Value of Extinction Coefficient Based on Improved Douglas-Peucker Algorithm

Ruonan Fei, Zheng Kong, Zhenfeng Gong, and Liang Mei*
Author Affiliations
  • School of Optoelectronic Engineering and Instrumentation Science, Dalian University of Technology, Dalian 116024, Liaoning, China
  • show less
    Figures & Tables(17)
    Picture of SLidar system
    Distribution of atmospheric echo signal measured by scanning SLidar system at different time. (a) 23:07, 2021-11-29; (b) 03:32, 2021-11-30; (c) 18:50, 2021-11-30; (d) 17:35, 2021-12-01
    Schematic of DP algorithm
    Flow chart of DP algorithm
    Flow chart for determining boundary value by DP algorithm and retrieving extinction coefficient
    Results of classical DP algorithm with different threshold values. (a)-(c) Lidar signal measured at 23:07, 2021-11-29; (d)-(f) lidar signal measured at 18:50, 2021-11-30
    Distribution of aerosol extinction coefficient retrieved by classical DP algorithm with different threshold values. (a), (c), (e) Distribution of aerosol extinction coefficient retrieved from lidar signals measured at 23:07, 2021-11-29; (b), (d), (f) distribution of aerosol extinction coefficient retrieved from lidar signals measured at 18:50, 2021-11-30
    Comparisons between target signal and reference signal measured at 23:07, 2021-11-29. (a) Lidar signals of target signal and reference signal; (b) reference signal and corresponding linear region found by DP algorithm; (c) linear regions found by classical DP algorithm with different threshold values for target signal; (d) comparisons between aerosol extinction coefficient profiles of target signal and reference signal
    Comparisons between target signal and reference signal measured at 18:50, 2021-11-30. (a) Lidar signals of target signal and reference signal; (b) reference signal and corresponding linear region found by DP algorithm; (c) linear regions found by classical DP algorithm with different threshold values for target signal; (d) comparisons between aerosol extinction coefficient profiles of target signal and reference signal
    Evaluation results by classical DP algorithm for lidar signals measured at different time. (a) 07:17, 2021-12-02; (b) 22:26, 2021-12-03
    Comparisons between target signal and reference signal measured at 07:17, 2021-12-02. (a) Lidar signals of target signal and reference signal; (b) reference signal and corresponding linear region found by DP algorithm; (c) linear regions found by improved DP algorithm with different threshold values for target signal; (d) comparisons between aerosol extinction coefficient profiles of target signal and reference signal
    Comparisons between target signal and reference signal measured at 22:26, 2021-12-03. (a) Lidar signals of target signal and reference signal; (b) reference signal and corresponding linear region found by DP algorithm; (c) linear regions found by improved DP algorithm with different threshold values for target signal; (d) comparisons between aerosol extinction coefficient profiles of target signal and reference signal
    Comparisons between aerosol extinction coefficients retrieved by classical DP algorithm and improved DP algorithm. (a) Retrieved aerosol extinction coefficients for lidar signal measured at 23:07, 2021-11-29; (b) retrieved aerosol extinction coefficients for lidar signal measured at 18:50, 2021-11-30
    Distributions of extinction coefficient at different time retrieved by improved DP algorithm. (a) 23:07, 2021-11-29; (b) 03:32, 2021-11-30; (c) 18:50, 2021-11-30; (d) 17:35, 2021-12-01
    Comparison between measurement results obtained from SLidar technique and air-pollution monitoring station. (a) Relative humidity measured by air-pollution monitoring station; (b) comparison between aerosol extinction coefficient evaluated from SLidar technique and PM10 concentration obtained from air-pollution monitoring station
    Scatter plot of PM10 concentration and aerosol extinction coefficient under different relative humidities (RHs). (a) RH higher than or equal to 60%; (b) RH less than 60%
    • Table 1. Parameter configurations of SLidar system

      View table

      Table 1. Parameter configurations of SLidar system

      ComponentModelSpecifications
      Laser sourceHigh-power diode laserWavelength 808 nm,output power 5 W
      CollimatorTianlang refractor telescopeFocal length 600 mm,diameter 100 mm
      ReceiverSkywatcher Newtonian telescopeFocal length 800 mm,diameter 200 mm
      DetectorLumenera CMOS camera Lt225NIRFrame rate 170 frame/s,bit depth 8 bit,resolution 2048 pixel×1088 pixel,tilt angle 45°
      Filters808 nm interference filter & SCHOTT RG 780 nm filterFull width at half maximum(FWHM)3 nm
    Tools

    Get Citation

    Copy Citation Text

    Ruonan Fei, Zheng Kong, Zhenfeng Gong, Liang Mei. Determination of Boundary Value of Extinction Coefficient Based on Improved Douglas-Peucker Algorithm[J]. Chinese Journal of Lasers, 2023, 50(14): 1410002

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category: remote sensing and sensor

    Received: Aug. 11, 2022

    Accepted: Sep. 22, 2022

    Published Online: Jul. 10, 2023

    The Author Email: Liang Mei (meiliang@dlut.edu.cn)

    DOI:10.3788/CJL221138

    Topics