ABSTRACT - DRUM - University of Maryland
ABSTRACT - DRUM - University of Maryland
ABSTRACT - DRUM - University of Maryland
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Troposphere Exchange Project (STEP/Tropical) showed the same result as in WVEE,<br />
observing tropospheric air penetrating and mixing into the stratospheric air.<br />
It seems clear that penetrative overshooting clouds do exist. However, the<br />
question <strong>of</strong> their frequency, i. e. whether this kind <strong>of</strong> overshooting occurs <strong>of</strong>ten enough<br />
to generate significant dehydration, is still unanswered. Recent work suggests that<br />
tropical convection is generally capped at altitudes 2-4 km below the tropical coldpoint<br />
tropopause, so there is only infrequent penetrative overshooting that reaches to<br />
the tropical tropopause level [Highwood and Hoskins, 1998; Folkins et al., 1999; Keith,<br />
2000; Gettelman et al., 2001].<br />
Sherwood and Dessler [2000, 2001] extended this convective dehydration<br />
hypothesis, and suggested a dehydration model by convective detrainment mixing into<br />
the TTL. In this TTL hypothesis, air is dehydrated rapidly as suggested by Danielsen<br />
[1982] but detrains at variable levels throughout the depth <strong>of</strong> the TTL. The bottom <strong>of</strong><br />
the TTL is close to the typical level <strong>of</strong> neutral buoyancy (LNB) <strong>of</strong> tropical convection<br />
[Selkirk, 1993]. Air detraining near the bottom <strong>of</strong> the TTL will have typical values <strong>of</strong><br />
water vapor mixing ratio (10-15 ppmv), which is relatively moist compared to the<br />
stratosphere. Air detraining at higher altitudes, however, must have originated in more<br />
energetic and warmer updrafts and/or overshot significantly. This air can be<br />
dehydrated to moisture levels far below average for the TTL.<br />
This newly dehydrated air, provided by overshooting clouds, spreads<br />
horizontally from the convective region, then mixes with moister air that detrained<br />
earlier at lower altitudes and has slowly risen to this altitude. Air on any given θ<br />
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