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<br />constants of nucleation. Their nucleation rate is dependent on Brmmian coagu- <br />lation which is a function of temperature and the size and concentration of both <br />the silver iodide aerosols and cloud droplets. They showed that at temperatures <br />warmer than -16 oC it takes from about 15 min to 1 h for 90 percent of the <br />silver iodide-silver chloride aerosols to nucleate ice crystals by the contact- <br />freezing mode, the exact times being dependent on the specific chemical com- <br />positon and cloud chamber conditions used. At temperatures colder than -16 oC, <br />DeMott et al. concluded that the deposition nucleation mode was dominant with <br />even longer nucleation time constants. These findings are generally consistent <br />with field observations (Dye et al., 1976; Strapp et al., 1979; English and <br />Marwitz, 1981) which report activation of ice crystals following silver iodide <br />seeding for 15 min and longer. <br /> <br />Seeding agents such as silver iodide-sodium iodide and silver iodide- <br />potassium iodide which appear to act by the condensation-freezing mode of <br />nucleation have somewhat shorter nucleation time constants. Blumenstein et <br />al. (1983) report that a silver iodide-sodium iodide nucleant produces 90 <br />percent of its ice crystals in about 14 to 20 min depending on temperature, <br />in a cloud chamber at water saturation. However, when subjected to tran- <br />sient supersaturations with respect to water, both the nucleation rate and <br />effectivity of the nucleant increased. In supersaturated conditions this <br />nucleant produced 90 percent of its ice crystals in about 4 min and its <br />effectivity increased by almost one order of magnitude. Rilling et al., <br />(1984) found that a silver iOdide-potassium iodide nucleant behaves simi- <br />larly. Finnegan et ale (1984) showed that the incorporation of a <br />hygroscopic salt, like sodium chloride, into the silver iodide-silver <br />chloride nucleus composition changed its mode of nucleation from contact to <br />condensation-freezing, thereby increasing both its effectivity and <br />nucleation rate, especially under transient supersaturation conditions. <br /> <br />The combined effects of a silver iodide seeding agent's nucleation rate and <br />residence time in a cloud is to make the nucleant's ice crystal yield less <br />than its effectivity at all temperatures, the amount of reduction depending <br />on the mode of nucleation and the cloud conditions where and when <br />nucleation actually occurs. In effect it lowers the temperature threshold <br />of activity for most silver iodide seeding agents to about _90 to -10 oC. <br />These factors may help to explain the diverse results of some of the past <br />cloud seeding experiments. <br /> <br />c. Physical evaluation of experiments <br /> <br />HIPLEX-1 represents a significant advance in our ability to design, carry <br />out and evaluate a randomized seeding experiment to improve our <br />understanding of precipitation development in natural and seeded clouds. <br />It specified in advance and attempted to verify by observations during the <br />course of the experiment each step leading to additional precipitation from <br />seedi ng. It was simil ar in approach to experiments conducted by Braham et <br />al., (1957) and Bethwaite et al., (1966) but more of the steps in the chain <br />of physical events could be included because of recent developments 'in <br />observing, measuring and real-time data processing capabilities. <br /> <br />Among the important concepts that were employed, some for the first <br />time in weather modification, in designing, executing and evaluating <br />HIPLEX-1 are the following (Smith et al., 1984): <br /> <br />10 <br />