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ABSTRACT - DRUM - University of Maryland

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not quantitatively indicate the extent to which they are mixing with their environment.<br />

Global analyses <strong>of</strong> cloud height do exist [e.g., Gettelman et al., 2002]. These analyses<br />

usually use brightness temperature from satellites to infer cloud height. However, the<br />

conversion from brightness temperature to altitude is uncertain [Sherwood et al., 2004]<br />

and therefore conclusions reached from these analyses require independent verification.<br />

In this study, an alternative method is used to determine the height <strong>of</strong> convecting<br />

clouds, as well as how much they mix with air in the TTL.<br />

3.2 Data<br />

To study overshooting convection, the data from the Visible and Infrared<br />

Scanner (VIRS) [Kummerow et al., 1998] onboard the Tropical Rainfall Measuring<br />

Mission (TRMM) [Simpson et al., 1996] are utilized. Four time periods (January 1998,<br />

July 1998, January 1999, and July 1999) are used in the analysis. These years are<br />

characterized by winter and summer seasons from both an El Nino (1998) and La Nina<br />

year (1999). VIRS makes measurements at five wavelengths (0.63-, 1.6-, 3.75-, 10.8-,<br />

and 12.0- µm) with a horizontal resolution <strong>of</strong> 2 km at nadir. In this study, data from the<br />

0.63-, 3.75-, and 10.8-µm channels are used. In addition, the 2.5º × 2.5º surface<br />

temperature and relative humidity from National Center for Environmental Prediction<br />

(NCEP) reanalysis [Kalnay et al., 1996] are used as initial conditions <strong>of</strong> an adiabatic<br />

altitude model.<br />

46

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