Infrared and Laser Engineering, Volume. 52, Issue 1, 20220262(2023)

Influence of atmospheric models on the aerosol optical parameters inversion and classification

Yuanzu Wang1, Dongsong Sun1, Yuli Han1, Jun Zheng1, and Yiming Zhao2
Author Affiliations
  • 1School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
  • 2Beijing Research Institute of Telemetry, Beijing 100076, China
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    Figures & Tables(16)
    Methodological flow for studying the influence of atmoshpere model on the retrieval of aerosol optical parameters
    The use of different atmospheric models (GDAS and ERA5) for the case of the Lille site in France (8th May, 2020, 20:00 to 21:00 UTC) has an impact on the retrieval results. (a) Relative deviation of the atmospheric molecular number density; (b) Relative deviation of the aerosol extinction coefficient at 355 nm obtained by the Raman method; (c) Relative deviation of the aerosol backscatter coefficient at 355 nm obtained by the Raman method
    Mean relative deviation of aerosol extinction coefficient and molecular number density at 355 nm from four stations
    Relationship between the mean relative deviation of back-scatter coefficient and aerosol concentration
    Aerosol extinction coefficient obtained by Raman method using different atmospheric models
    Aerosol backscatter coefficient obtained by the Raman and elastic scattering methods using different models
    Aerosol lidar ratio and color ratio results of dual wavelength obtained by different atmospheric models
    Ångström exponent results retrieved by different atmospheric models
    48 h backward trajectory of aerosol provided by HYSPLIT model
    • Table 1. Mean and standard deviation of typical values of aerosol type related characteristics

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      Table 1. Mean and standard deviation of typical values of aerosol type related characteristics

      Type$ {S}^{355} $/sr $ {S}^{532} $/sr $ {\kappa }_{\alpha }\left({355,532}\right) $${\kappa }_{\beta }\left({355,1\;064}\right)$${\kappa }_{\beta }\left({532,1\;064}\right)$$ {\kappa }_{\beta }\left({355,532}\right) $
      CC50±841±61.7±0.61.0±0.21.0±0.31.3±0.3
      PC69±1263±131.7±0.51.3±0.31.3±0.21.4±0.6
      D58±1255±70.3±0.40.4±0.10.4±0.10.3±0.2
      MD42±447±60.5±0.30.5±0.20.4±0.30.7±0.3
      PD54±864±90.6±0.20.9±0.30.8±0.11.0±0.5
      MM25±724±80.9±0.30.8±0.10.8±0.21.0±0.3
      S81±1678±111.3±0.31.3±0.11.3±0.11.2±0.3
      V50±1148±130.2±0.30.1±0.10.4±0.30.2±0.3
    • Table 2. Basic information of EARLINET observing stations

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      Table 2. Basic information of EARLINET observing stations

      LidarElastic scattering/nmRaman/nmInstitution
      3555321 064387607530
      MUSACNR-IMAA, Potenza, Italy
      LRD200
      PollyXTTROPOS, Leipzig, Germany
      PAOLIUniversidade de Évora, Portugal
      LILASUniversité de Lille, France
    • Table 3. Vertical pressure levels of different model data

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      Table 3. Vertical pressure levels of different model data

      DatasetVertical pressure levels
      ERA5137 vertical levels from the surface to 0.02 hPa
      IFS_ECMWF137 vertical levels from the surface to 0.01 hPa
      GDAS23 vertical levels from the surface to 20 hPa
    • Table 4. Maximum deviation of different models for aerosol extinction coefficient obtained by Raman algorithm at different wavelengths and corresponding deviation of molecular number density from four stations

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      Table 4. Maximum deviation of different models for aerosol extinction coefficient obtained by Raman algorithm at different wavelengths and corresponding deviation of molecular number density from four stations

      AlgorithmRaman method
      Wavelength/nm355532
      Maximum deviation ${{D} }_{\alpha }$20.43%19.44%
      Corresponding deviation $ {D}_{N} $0.59%0.44%
    • Table 5. Maximum deviation of different models for backscatter obtained by two algorithms at different wavelengths and corresponding deviation of molecular number density from four stations

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      Table 5. Maximum deviation of different models for backscatter obtained by two algorithms at different wavelengths and corresponding deviation of molecular number density from four stations

      AlgorithmRaman methodElastic scattering method
      Wavelength/nm3555323555321064
      Maximum deviation $ {D}_{\beta } $−2.22%−2.27%11.11%4.80%2.79%
      Corresponding deviation $ {D}_{N} $−2.29%−2.16%−2.02%0.20%1.56%
    • Table 6. Maximum deviation, mean value and standard deviation in the low aerosol concentration region (IB < 0.0015 sr −1) at three wavelengths from four stations

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      Table 6. Maximum deviation, mean value and standard deviation in the low aerosol concentration region (IB < 0.0015 sr −1) at three wavelengths from four stations

      Statistics projectResults
      355 nm532 nm1064 nm
      Maximum deviation11.11%4.8%2.79%
      Mean value4.26%1.58%0.74%
      Standard deviation2.80%1.27%1.24%
    • Table 7. Mean value and standard deviation of related parameters of aerosol type using different atmospheric models at an altitude of 1.5-2 km

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      Table 7. Mean value and standard deviation of related parameters of aerosol type using different atmospheric models at an altitude of 1.5-2 km

      ModelRelated parameters
      $ {\mathrm{\kappa }}_{\alpha }\left(\mathrm{355,532}\right) $$ {\mathrm{\kappa }}_{\beta }\left(\mathrm{355,532}\right) $${\mathrm{\kappa } }_{\beta }\left(\mathrm{355,1\;064}\right)$${\mathrm{\kappa } }_{\beta }\left(\mathrm{532,1\;064}\right)$$ {S}^{355} $/sr $ {S}^{532} $/sr ${ {Y} }\left(\mathrm{532,355}\right)$
      GDAS0.9±0.31.2±0.21.1±0.11.0±0.136±240±71.1±0.2
      ERA50.8±0.31.2±0.21.1±0.11.0±0.139±245±61.1±0.2
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    Yuanzu Wang, Dongsong Sun, Yuli Han, Jun Zheng, Yiming Zhao. Influence of atmospheric models on the aerosol optical parameters inversion and classification[J]. Infrared and Laser Engineering, 2023, 52(1): 20220262

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    Paper Information

    Category: Atmospheric optics

    Received: Apr. 18, 2022

    Accepted: --

    Published Online: Feb. 9, 2023

    The Author Email:

    DOI:10.3788/IRLA20220262

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