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<br />over the Mesa in a more direct fashion. Similar effects were <br />observed on the north side of the Mesa, with northwest <br />winds; the lower winds became perpendicular to the Mesa <br />as they approached it. Even southwest flow entering the <br />"convergence notch" between the arms of the Mesa probably <br />crosses the Mesa and descends on the north side relatively <br />quickly. This rapid transit and descent may pose a targeting <br />problem, as the time available for newly nucleated crystals <br />to grow in a SLW-rich environment will be relatively short, <br />about 30 minutes, given an average cross-barrier wind com- <br />ponent of 10 m/s. <br /> <br />None of the aircraft LWC data were collected during any of <br />the 23 previously-identified episodes of heavy SL W, although <br />2 flight~ were made in conditions that later developed into <br />major episodes. Most of the heavy SLW episodes occurred <br />with GJT 70-kPa winds from more southerly directions than <br />cases sampled by the aircraft. Significant icing did occur on <br />several occasions, and in one instance a flight was terminated <br />due to heavy airframe icing, which suggests that some re- <br /> <br />search aircraft may not be able to remain on station during <br />the heaviest SLW episodes. <br /> <br />2.4.2 Radar Measurements. - Hourly averages of cloud tops <br />measured by a Ka-band radar at the Island Lake Site were <br />plotted against SLW for January through March 1985 (fig. <br />2-5). Echoes were subjectively classified as either stratiform <br />or convective based on the appearance of the facsimile trace <br />produced by the radar. Those echoes classified as convective <br />were primarily embedded convection. <br /> <br />With only two exceptions, SLW amounts greater than <br />0.5 mm were observed during convective periods, and were <br />associated with cloud tops between 4 and 6 km m.s.!. Few <br />tops higher than 6 km were observed. <br /> <br />A least-squares fit to figure 2-5 produced a correlation coef- <br />ficient of 0.22 and a slope of + 1.08, showing only a weak <br />(though positive) relationship between cloud top height and <br />SLW. <br /> <br />8.0 <br /> <br /> <br /> . . <br /> .. . . . <br /> . . <br />. . 0 <br /> 0 . <br /> . . . . . <br /> . .. . <br /> . <br /> .. . . <br />0 . <br /> .. . <br />0 <br /> Water <br /> <br />u) <br />E <br />E <br />~ <br /> <br />7.0 <br /> <br />(f) <br />a. <br />06.0 <br />~ <br /> <br />. <br />o 0.. <br />o ... <br /> <br /> <br />. <br /> <br />o 0 0 . <br /> <br />""0 <br />::::J <br />o <br />U <br /> <br />""0 5.0 <br />c: <br />IV <br />a:l <br />leu <br />~ <br /> <br />oe . . <br />. III . <br /> <br />o O. <br />. <br /> <br />o <br />0..0 . <br />. . <br /> <br />o <br /> <br />. <br />. 0 <br />o ~ .0 <br />. <br /> <br />o 0 <br /> <br />. .. <br /> <br />o . <br /> <br />3.5 <br />0.0 <br /> <br />· Convective 12641 <br />HOURLY AVERAGES 0 Stratiform 14611 <br /> <br />o <br /> <br />. <br /> <br />. . <br /> <br />. tt <br />. <br />. . <br /> <br /> <br /> <br />Figure 2-5. - Hourly averages of Ka-band cloud tops plotted against SLW. The greatest amounts of SLW were observed during convective <br />periods. Few cloud tops higher than 6 km m.s.l. were observed. <br /> <br />9 <br />