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<br />. <br /> <br />estimated using the technique described by Paluch (1979). The potential <br /> <br />for the formation of penetrative downdrafts, via mixing of <br /> <br />. <br /> <br />environmental air through cloud top and evaporative cooling, was <br /> <br />addressed using the potential buoyancy plots found in Cooper et al. <br /> <br />(1982b,c) . These diagrams used composite aircraft soundings near the <br /> <br />. <br /> <br />target cloud to assess the maximum negative buoyancy possible from <br /> <br />mixing cloudy air (containing adiabatic liquid water content) with <br /> <br />envirorunental air until all of the cloud liquid water was evaporated. <br /> <br />. <br /> <br />Fig. 2.15 is a composite of the maximum negative buoyancies for the <br /> <br />20 HIPLEX-l clouds. Also shown is a representative temperature scale <br /> <br />and the adiabatic liquid water content assuming a cloud base pressure <br />of 700 rob and temperature of 30C. The data in this figure show that a <br /> <br />. <br /> <br />strong potential for the formation of negative buoyancy exists in <br />200 <br /> <br />300 <br /> <br /> <br />. <br /> <br />400 <br /> <br />:0 <br />E 500 <br />w <br />a:: 600 <br />:J <br />U) <br />U) <br />w <br />a:: 700 <br />a. <br /> 800 <br /> 900 <br /> 1000 <br /> -4 -2 0 2 4 <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />T-Tenv (OC) <br /> <br />LIQUID WATER CONTENT (g/m&) <br />Fig. 2.15: Composite of the potential negative buoyancy plots for the 20 <br />HIPLEX-l clouds. The minimum potential buoyancy results from mixing of <br />the adiabatic parcel with envirorunental air at the indicated altitude <br />in the proportion required to just evaporate the liquid water in the <br />cloud parcel. A representative envirornnental temperature scale is <br />shown, and the adiabatic liquid water content expected for cloud base <br />pressure of 700 rob and temperature of +30C is also plotted (LWCAD). <br /> <br />24 <br /> <br />. <br /> <br />. <br />