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<br />1764 <br /> <br />JOURNAL OF APPLIED METEOROLOGY <br /> <br />VOLUME 17 <br /> <br /> 10 <br /> 9 <br /> 8 <br /> 7. <br />E <br />.x <br /> 6 <br />:r: <br />l- <br />e.. <br />w 5 <br />0 <br />0 <br />::J 4 <br />0 <br />-' <br />u <br /> 3 <br /> 2 <br /> <br />~ ~~~ ~~ ~ <br /><:> V' ,0 V' nO V' 0.0 V' -00 V' 00 V' 00 V' <br />.. ~ 'lJ 0. <br />15 1510 5 <br /> <br /> <br />I 2 3 4 5 6 7. 8 9 10 <br /> <br />15 <br />UPDRAFT (m s-I) <br /> <br />-150 C <br /> <br />50C <br /> <br />8m= 23, 20C <br />BASE=3km <br />M.R. = 11.3 g kg-I <br /> <br />20 <br /> <br />25 <br /> <br />30 <br /> <br />FIG. 5. As in Fig. 4 except for cooler, drier cloud. <br /> <br />30 <br /> <br />51""INITIAL SIZE <br />em~23.2.C <br />BASE ~ I km <br />MR~16.2 9 kg-I <br /> <br />- -- - 51""INITIAL S'ZE <br />em ~ 16.C <br />BASE~2km <br />M.R.~7.6g kg-" <br /> <br />E <br />.5. <br /> <br /> <br />20 <br /> <br />25 <br /> <br />o <br />w <br />~ 20 <br />f'! <br />I- <br />'" <br /> <br />a: <br />w 15 <br />I- <br />w <br />" <br />'" <br /><3 <br />" <br />::> <br />" <br />X 10 <br />'" <br />" <br /> <br />.......... <br />/ \ <br />I \ <br />I \ <br />I \ <br />I \ <br /> <br />10 15 <br />UPDRAFT (m ,-II <br /> <br />FIG. 6. Variation of the maximum drop size attained as a <br />function of updraft speed for initial hygroscopic drop diameter <br />of 5 ILm for moist and relatively dry cloud conditions (model <br />computation). <br /> <br />25 <br /> <br />5. Comparative analyses <br /> <br />a. Comparison with natural embryos and AgI nuclei <br /> <br />Prior to seeding, a determination has to be made <br />of the suitability of a particular day for hygroscopic <br />seeding. Even if a given day is considered suitable, <br />it may well be that only clouds that have specific <br />physical characteristics are deemed seedable. Such <br />parameters as cloud-base height and temperature, <br />cloud thickness and diameter, updraft and cloud-water <br />profiles, and cloud droplet spectra all play a very <br />important role in determining' the efficiency with <br />which hygroscopic seeds will act to stimulate addi- <br />tional precipitation from a cloud. <br />It is a very difficult task to determine just how <br />much help a particular seeding effort may have con- <br />tributed to the total precipitation from a cloud system. <br />There are still many uncertainties to be resolved <br />before this problem is solved. For instance the sto- <br />chastic theory for the production of large droplets <br />(> 100 ~m) does not always adequately explain the <br />formation of these droplets in the times observed. <br />In-cloud measurements have shown particles of this <br />general size to already exist at cloud base in concen- <br />trations of 0.5 to 1.0 e-I in Texas, Ariwna and South <br />Dakota (Takeuchi, 1972). Others have also found <br />evidence of the existence of large cloud droplets <br />(40-100 ~m) near the bases of cumulus clouds (e.g., <br />Ludlam, 1959; MacCready and Takeuchi, 1968; <br />Kopcewicz, 1965; Rosinski and Kerrigan, 1969). Ac- <br />cordingly, it might be more appropriate in the present <br />