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<br />The ice crystals required for the formation of natural precipi- <br />tation are produced when freezing or sublimation nuclei become ef- <br />fective at existing cloud temperatures, or when ice crystals are <br />introduced directly into the cloud volume from external sources (e.g., <br />natural seeding from nearby clouds containing ice). <br />Supercooled shallow orographic cloud systems over the High Plains <br />often produce little or no precipitation. These clouds are thought to <br />produce little natural precipitation because of their shallowness, be- <br />cause of the low concentrations of natural ice nuclei active at pre- <br />vailing cloud temperatures, and because of the inefficiency of the <br /> <br />warm rain coalescence process. <br /> <br />On the other hand, the artificial production of significant pre- <br />cipitation from these cloud systems is favored by: <br />1. A temperature range where their precipitation potential <br />can be released artificially through seeding. <br />2. The high frequency of these clouds in the High Plains region, <br />3. The widespread nature of these cloud systems, and <br />4. Their relatively long duration. <br />Physical and numerical models have recently been developed for <br />cold orographic cloud systems in the western mountains of the U. S. <br />(e.g., Chappell, 1970; or Willis, 1970). These models, with some modifi- <br />cations, can be adapted to the shallow orographic cloud systems of the <br />High Plains. <br />Although the seedable cloud systems in the High Plains are similar <br /> <br />1 <br />, I <br />! <br /> <br />in some respects to those on the western mountain ranges, some <br /> <br />2 <br />