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Original Articles

Aerosol Properties Computed from Aircraft-Based Observations During the ACE-Asia Campaign: 2. A Case Study of Lidar Ratio Closure

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Pages 231-243 | Received 20 Feb 2006, Accepted 30 Nov 2006, Published online: 17 Jan 2007

Figures & data

FIG. 1 (left) Vertical profile of aerosol extinction at different wavelengths, derived from sunphotometer measurements on April 17 (CitationSchmid et al. 2003). (middle) Vertical profiles of the lidar ratio derived from sunphotometer/lidar measurements (implied lidar ratio) (CitationSchmid et al. 2003), and the lidar ratios calculated from the retrieved and in-situ measured size distributions. The error bars in the lidar ratios modeled from the measured size distributions are due to uncertainties in size distributions and real part of refractive index. (right) The lidar ratio modeled profiles which correspond to single scattering albedo values of 0.88 and 0.98 in the boundary layer, 0.88 and 0.94 in the pollution layer, and 0.92 and 0.96 in the dust layer.

FIG. 1 (left) Vertical profile of aerosol extinction at different wavelengths, derived from sunphotometer measurements on April 17 (CitationSchmid et al. 2003). (middle) Vertical profiles of the lidar ratio derived from sunphotometer/lidar measurements (implied lidar ratio) (CitationSchmid et al. 2003), and the lidar ratios calculated from the retrieved and in-situ measured size distributions. The error bars in the lidar ratios modeled from the measured size distributions are due to uncertainties in size distributions and real part of refractive index. (right) The lidar ratio modeled profiles which correspond to single scattering albedo values of 0.88 and 0.98 in the boundary layer, 0.88 and 0.94 in the pollution layer, and 0.92 and 0.96 in the dust layer.

TABLE 1 Uncertainties in in-situ measured aerosol size distributions (CitationWang et al. 2002) (note that these uncertainties do not include uncertainties associated with adjustment to ambient RH)

FIG. 2 (top) Comparison of size distribution retrieved from the sunphotometer-derived aerosol layer optical thickness spectrum, with the layer-averaged in-situ measured size distribution in the pollution layer (CitationKuzmanoski et al. 2006). (bottom) Corresponding extinction and backscattering contribution functions R.

FIG. 2 (top) Comparison of size distribution retrieved from the sunphotometer-derived aerosol layer optical thickness spectrum, with the layer-averaged in-situ measured size distribution in the pollution layer (CitationKuzmanoski et al. 2006). (bottom) Corresponding extinction and backscattering contribution functions R.

FIG. 3 (top) Comparison of size distribution retrieved from the sunphotometer-derived layer aerosol optical thickness spectrum, with the layer-averaged in-situ measured size distribution in the dust layer (CitationKuzmanoski et al. 2006). (botto m) Corresponding extinction and backscattering contribution functions.

FIG. 3 (top) Comparison of size distribution retrieved from the sunphotometer-derived layer aerosol optical thickness spectrum, with the layer-averaged in-situ measured size distribution in the dust layer (CitationKuzmanoski et al. 2006). (botto m) Corresponding extinction and backscattering contribution functions.

TABLE 2 Aerosol size-dependent refractive indices based on aerosol chemical analysis (CitationWang et al. 2002), in three layers observed in the vertical profile of April 17, and average lidar ratio values calculated from retrieved and measured size distributions.

TABLE 3 Uncertainties in calculated lidar ratios in three observed layers in the aerosol profile observed on April 17, 2001

FIG. 4 Comparison of size distributions, derived using LUT and constrained linear inversion methods from the sunphotometer-derived extinction and corresponding extinction spectra at the altitude h = 0.63 km.

FIG. 4 Comparison of size distributions, derived using LUT and constrained linear inversion methods from the sunphotometer-derived extinction and corresponding extinction spectra at the altitude h = 0.63 km.

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