Full text: XIXth congress (Part B7,3)

  
Poli, Daniela 
  
The resulting y-parallaxes are a function of the height, the along-track wind component (only for clouds) and of the nadir 
and forward zenith angle. The nadir and forward zenith angle are known at 11 equally distributed points of the first and 
last scan line from the GBT header and can be linearly interpolated for all pixels (Bailey, 1995). If no cloud motion 
information is available, the cloud height 4 is calculated from the uncorrected y-parallax y, after (Prata and Turner, 
1997): 
= Yp 
tan((x,) — tan(x,)) N 
where x; x, forward/nadir zenith angle 
yp: parallax in y-direction 
If either the cloud wind vector or the total cloud wind velocity is available from another source (e.g. Meteosat cloud 
winds), the y-parallax can be corrected for the wind-induced along-track amount. The x-parallax is a function of the 
across-track wind component and of the resampling error (for gridded products). For the wind corrections, the exact time 
difference between the same pixel in the forward and the nadir scan has to be calculated from the along-track distance 
and the satellite velocity. 
4 CONCLUSIONS 
The potential of deriving cloud-top heights from stereo satellite images with 288 m and 1000 m resolution has been 
demonstrated. The same algorithms could be used with both datasets. Preprocessing and post-processing blunder 
detection algorithms led to improvements. The accuracy potential of our matching approach, as shown with the MOMS 
data, is well into the subpixel range, being able to fulfil the accuracy requirements for applications in weather and 
climate. Similar matching problems were encountered, with slightly more for MOMS due to the larger parallax range and 
higher resolution. Large blunders remain undetected in the results, caused mainly by the surface discontinuities, mixing 
of image neighboring areas of large vertical separation, reflectance differences, and poor approximate values. 
Approaches to reduce these problems have been already identified and will be implemented in future investigations. 
ACKNOWLEDGEMENTS 
We would like to thank Dirk Stallmann, Institute for Photogrammetry, University of Stuttgart for providing valuable help 
in processing of the MOMS-02 imagery and Chris Mutlow, Rutherfold Appleton Laboratory, for valuable comments 
about the ATSR2 data. The ATSR2 data was kindly provided by the ESA NRT service. 
This work is funded by the Bundesamt für Bildung und Wissenschaft (BBW) within the EU-project CLOUDMAP (BBW 
Nr. 97.0370). 
REFERENCES 
Bailey, P., 1995. SADIST-2 v100 products. ER-TN-RAL-AT-2164, Rutherford Appleton Laboratory. 
Baltsavias, E.P., 1991. Multiphoto geometrically constrained matching. Ph. D. dissertation, Institute of Geodesy and 
Photogrammetry, ETH Ziirich, Mitteilungen No. 49, 221 p. 
Baltsavias, E. P, Stallmann, D., 1996. Geometrical potential of MOMS-02/P data for point positioning, DTM and 
orthoimage generation. IAPRS, Vol. 31, Part B4, pp. 110 - 116. 
Buongiorno, A., 1999, WWW ATSR Near Real Time service, quick guide, version 1.0. ESA/ ESRIN. 
Danson, F.M., Higgins, N.A., Trodd, N.M., 1999. Measuring land-surface directional reflectance with the along-track 
scanning radiometer. Photogrammetric Engineering and Remote Sensing, 65 (12), pp. 1411-1417. 
  
1168 International Archives of Photogrammetry and Remote Sensing. Vol. XXXIII, Part B7. Amsterdam 2000.
	        
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