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Results

Data was acquired at UW - Madison (96 N, 32 W) during simultaneous operation of HSRL and AERI systems; where each case includes a local CLASS radiosonde launch, see Table 3 for summary. HSRL data sets were typically scheduled to coincide with a satellite measurement (Landsat, NOAA-11 overpass, or GOES-8 scan). It should be noted that the UW Volume Imaging Lidar (VIL) (Piironen and Eloranta, 1995) was also in operation on various days.  

 
Date
Time (UTC)
Cloud Description
17 Nov 1994
00:00-05:15
Scattered cirrus, 7.5 to 12 km.
25-26 Oct 1995
22:00-02:00
Mostly clear, some thin scattered
cirrus, 9-11 km.
26 Oct 1995
14:15-19:00
Thick ice cloud with base at 2 km, turning to
mixed phase at 4 km, then back to ice.
9-10 Nov 1995
23:30-03:00
Moderate cirrus, increasing in optical thickness
with decreasing cloud base.
16-17 Nov 1995
22:00-02:45
Clear skies turning cloudy with non-uniform
cirrus above a thin layer of water.
2 Dec 1995
18:15-19:15
4 km water cloud with very uniform base.
Broken cirrus noted at 6 to 8 km.
4 Dec 1995
15:15-20:00
Broken cirrus, some water, very
non-uniform cloud.
6 Dec 1995
16:15-23:00
Broken, thin cirrus at 6-10 km, becoming clear.
Table 3: AERI/HSRL Data Cases at UW - Madison

Derived results for each instrument are classified into two categories: optical depth and brightness temperature. Optical depth calculations yield a visible to infrared optical depth ratio, tex2html_wrap_inline3093, that is based on a uniform infrared cloud extinction cross-section. Brightness temperature measurements utilize a weighted visible cloud extinction cross-section to derive tex2html_wrap_inline3095. The goal is to demonstrate the improvement gained in using the latter approach. This will illustrate agreement between the instruments, while taking care to differentiate inconsistencies due to errors associated with instrument properties and measurements, atmospheric conditions, and assumptions inherent in the incorporation of FASCOD3P and Mie model simulations.

In an effort to avoid confusion from multiple data sets, emphasis will be placed on results from two cases. Data from these days is useful in that the data acquisition period extended for several hours; and the observations were comprised of cirrus over a range of optical thickness and cloud base altitudes. Figures 10 through 13 illustrate the inverted HSRL aerosol backscatter and depolarization for these cases.

Figures 10 and 11 are inverted aerosol backscatter and depolarization, respectively, for data taken on 17 November 1994. Times are given in Universal Coordinated Time (UTC). Data is displayed in range-time-indicator (RTI) format, where the backscatter intensity scale is given in the color bar to the right of the image. Broken cirrus exists between 7 and 12 km, which provides a variable case for comparison against the AERI data. The feature within the bottom 2 km of the RTI is the planetary boundary layer. Large depolarization values, Figure 11, shows the clouds to consist entirely of ice particles. Depolarization remains near zero for spherical particles, which are seen within the humid boundary layer. This agrees with the radiosonde data which was previously shown in Figure 2.

Figures 12 and 13 are inverted aerosol RTIs for 9-10 November 1995. Two features make this an interesting case for study: the cloud base continues to decrease, nearly monotonically, over a 4 km range in a period of 2 hours; and the optical depth increases until it becomes opaque, with respect to the lidar, near 01:30 UTC. The moderate, boundary level aerosol layer depolarization near 1 km, Figure 13, indicates a transformation from spherical to non-spherical particles between 01:00 to 02:00 UTC.

   figure917
Figure 10: HSRL inverted aerosol backscatter signal for 17 November 1994. The abscissa indicates time in UTC format.

   figure923
Figure 11: HSRL inverted aerosol depolarization signal for 17 November 1994. The abscissa indicates time in UTC format.

   figure929
Figure 12: HSRL inverted aerosol backscatter signal for 10 November 1995. The abscissa indicates time in UTC format.

   figure935
Figure 13: HSRL inverted aerosol depolarization signal for 10 November 1995. The abscissa indicates time in UTC format.



next up previous
Next: AERI and HSRL Derived Optical Depth Up: Abstract and Contents Previous: CLASS

Daniel DeSlover
Sun Aug 11 10:02:40 CDT 1996