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<br />ice nuclei into clouds and the scientific exploration of the weather modi- <br />fication possibilities envisoned earlier could begin. Field experiments on <br />artifically stimulating rain from convective clouds based on the Bergeron <br />process began almost immediately (e.g., Kraus and Squires, 1947; Leopold <br />and Halstead, 1948; Squires and Smith, 1949; Smith, 1949). <br /> <br />The static seeding hypothesis for convective clouds is based on obser- <br />vations that precipitation development in these clouds is frequently inef- <br />ficient and on the expectation that the natural precipitation process can <br />be made more efficient by the introduction of additional precipitation <br />embryos through glaciogenic seeding. The presence of supercooled water and <br />concomitant low concentrations of ice particles at temperatures wamler <br />than about -20 oC are generally taken as evidence of the inefficiency of <br />the precipitation process. The static seeding strategy is to provide an <br />optimum concentration of ice particles for the available liquid water and <br />initiate the precipitation process earlier and, perhaps, lower in altitude <br />in the developing cloud than would occur naturally. Attaining on the order <br />of 1 to 10 ice crystal s per 1 iter that eventually woul d become 0.1 to 1.0 <br />graupel embryos per liter is the usual goal of the seeding operation. If <br />too many ice crystals for the available water are produced then none! may <br />grow large enough to fallout and the cloud is said to be "overseede!d" <br />(Bergeron, 1949). <br /> <br />Static seeding is intended to improve the precipitation efficiency of a <br />cloud by affecting its microphysical properties only. Changes in the dyna- <br />mical properties of the clouds may occur, but they are neither intended nor <br />part of the cause-and-effect relationship in the seeding hypothesis. <br /> <br />3 <br />