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<br />chilled by evaporation; hence it was the negatively buoyant, descend- <br />ing air into which the latent heat of fusion was released, thus <br />detracting from the total circulation and dumping most of the silver <br />iodide into downdraft or detritus regions. Only much later would <br />some portion of the silver iodide find its way by further mixing <br />into the central updraft, by which time the cloud would have passed <br />its phase of active growth and be dissipating. Thus the model pro- <br />vides a framework for reasoning that the ARIDROP treatment contrib- <br />uted to growth of the treated cloud and the Catalina treatment to <br />its dissipation. <br /> <br />This reasoning is in general agreement with the outcome not only of <br />the Flagstaff versus the Catalina experiments but also of a consid- <br />erable number of others where, on the one hand silver iodide was <br />released directly into the updrafts of clouds selected for their <br />suitability (e.g., Bethwaite, et aI, 1966; Henderson, et aI, 1968) <br />and on the other hand the treatment was simi lar to that of Catalina <br />(e.g., Godson, et aI, 1966; Decker & Schickedanz, 1967; Decker. et <br />ai, 1971; Smith, 1967). If one extends the comparison further by <br />assuming that silver iodide seeding from ground-based generators, <br />by dispersing the nucleant from the source level of cloud-building <br />heat and moisture, results in selective uptake of nucleant into the <br />strongest cloud-building updrafts (Howell, 1966), and hence that <br />this procedure more nearly resembles the Flagstaff than the Catalina <br />treatment as it affects cloud dynamics, then the area of general <br />agreement between the prediction and experience is widened and a <br /> <br />7 <br />