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<br />- !i3 - <br /> <br />Particles with molecular spacings and crystallographic arrangements similar to those of ice <br />(which has a hexagonal structure) tend to have good ice nucleating properties and a high <br />threshold temperature. Most good ice nuclei are also virtually insoluble. Table 1 gives the <br />threshold temperatures and the structure of some natural and artificial ice nuclei. <br /> <br />Table 1: Crystallographic structure and threshold temperatures of <br />some natural and artificial ice nuclei <br /> <br />natural IN artificial IN <br />Covellite hexagonal -60 C Ag I hexagonal -40 C <br />Tridymite hexagonal -7D C Pb 12 trigonal -40 C <br />Kaolinite tric linic -90 C Cu S hexagonal _60 C <br />Magnetite cubic -90 C Methaldehyde tetr-lo C <br /> <br />Many organic materials are good ice nucleators. The University of Wyoming group has recently <br />discovered that decayed biological matE'rial contains copious ice nuclei (see Vali et al.. <br />1976). In weather modification pyrotechnics of Ag I and Pb 12 are widely used as seeding <br />material. In order to disperse them in a cloud. a direct injection technique should be used, <br />since there is evidence (Federer et al.. 1979) that the nuclei are deactivated in the warm <br />parts of the cloud due to the blocking of active nucleation sites by impurities of the <br />pyrotechnics. <br /> <br />Measurement of IN <br /> <br />Several techniques exist for measuring the concentrations of IN. A common method is to <br />draw a known volume of air into a contcliner and to cool it until a cloud is formed (Fig. 7). <br />The number of ice crystals forming at CI particular temperature is then measured. In <br />expansion chambers the cooling is produced by compressing the air and then suddenly expand- <br />ing it, and in mixing chambers cooling is produced by refrigeration. In these chambers. <br />particles may serve as freezing, contact or deposition nuclei. In laboratory investigations <br />on artificial nuclei it is sometimes possible to distinguish between these 3 mechanisms <br />(Langer et al., 1978). The number of ice crystals which appear in the chamber may be deter- <br />mined by illuminating a certain volume of the chamber and estimating visually the number of <br />ice crystals in the light beam. by letting the ice crystals fall into a dish of supercooled <br />sugar solution where they can be detected and counted by the number of larger crystals that <br />they produce, or by allowing the ice crystals to pass through a small capillary tube <br />attached to the chamber, where they produce audible clicks which can be counted electronic- <br />ally (Langer. 1973). In another technique. a measured volume of air is drawn through a <br /> <br />Sugar solution <br />In tray <br /> <br /> <br />Lid clamp <br /> <br />-~-- <br /> <br />Air <br />intake <br /> <br />Fig. 7: Schematic design of thH U.S. Weather Bureau version of a Bigg-Warner box <br />(From Byers, 1965). <br />