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<br />7.3 Key Physical Findings <br /> <br />Brief answers to the above questions, based largely on the work reported herein, are now stated: <br /> <br />a. A considerable body of evidence from the Plateau investigations and some other work shows that <br />significant SLW cloud exists over western mountains in excess of that naturally converted to ~ <br />snowfall. This "excess" SL W flux represents a large fraction of seasonal snowfall amounts. <br />While the existence of "excess" SL W water cloud has been assumed for decades, aqd is necessary <br />for operational seeding to have any potential, adequate documentation has been provided only <br />during the past several years. Field deployment of microwave radiometers has been especially <br />important in this documentation. ' <br /> <br />b. Orographic cloud SL W varies rapidly in time and space. Some of the greatest SL W amounts have <br />been found during storms with strong synoptic support which are naturally very efficient snow <br />producers during some phases but inefficient during other phases. Conversely, weaker localized <br />storms typically produce lesser SL W amounts but these persist over many hours per winter. Both <br />storm types are important in total seasonal SL W flux production. <br /> <br />"'. <br /> <br />c. Orographic cloud SL W is usually found over the windward slopes and crests and rapidly <br />diminishes further downwind, even as cloudy air moves across the relatively flat Plateau top, <br />about 10 kIn wide. The SL W is depleted by a combination of snowfall production and subsidence <br />of the airflow. <br /> <br />d. The SL W cloud is confined to a shallow layer above the terrain. Most SL W condensate exists in <br />the lower 500 m above the terrain and SL W amounts are usually' negligible at an altitude of <br />1,000 m above the terrain. Forced orographic uplift, weak embedded convection, and gravity <br />waves all combine to produce the liquid condensate. <br /> <br />e. The SL W cloud found near the mountainous terrain is typically mildly supercooled over Utah's <br />mountains. Frequently, the SL W cloud is too warm for significant ice nucleation with AgI, except <br />perhaps in its upper portions. Often natural ice nucleation processes become efficient as cloud <br />temperatures become cold enough for effective AgI nucleation. Consequently, the "window of <br />opportunity" for effective AgI seeding is limited to a fraction of the periods with "excess" SL W. <br />To restate this important point, most SL W periods cannot be effectively seeded with the present <br />type of operationally applied AgI, especially when it is released from the ground with resulting <br />limited vertical dispersion. <br /> <br />f. The frequency of successful transport of AgI plumes over the Plateau is directly related to <br />generator elevation relative to the mountain barrier. Plumes released from high altitude sites <br />within 300 to 500 m of the Plateau top were routinely transported over the barrier when winds had <br />a cross-barrier component, necessary for significant SL W production. Similar results have been <br />demonstrated at several other mountainous locations, including Montana, Colorado, and Arizona. <br />High altitude release s.ites on the Plateau were usually just below or just ~bove cloud base. <br /> <br />. . <br /> <br />g. While experimental cases are limited, adefinite impression developed over the course of the <br />experiments that canyon mouth releases have a significantly greater probability of over-Plateau <br />tr:ansport than valley releases. <br /> <br />h. Plumes released from the valley floor are less likely to be transported over mountain barriers than <br />plumes released from higher elevation sites. . A number of experimental periods showed that AgI <br /> <br />30 <br /> <br />