Laserfiche WebLink
<br />II. CLOUD SEEDING AGENTS AND DELIVERY SYSTEMS 603 <br /> <br />substances have been used to produce the same <br />effect, including liquid propane, liquid air, and <br />solid objects previously chilled by immersion in <br />some very cold substance. The effect can also <br />be produced by decompression, as in an explo- <br />sion or at certain positions near some types of <br />aircraft in flight. <br />Although chilling agents must freeze preexist- <br />ing cloud droplets and activate additional nuclei, <br />these effects are insufficient to account for the <br />myriads of ice crystals produced. The vast ma- <br />jority of the ice crystals are produced by homo- <br />geneous nucleation from the vapor phase. It is <br />not completely settled whether they form by ho- <br />mogeneous deposition from vapor to ice or <br />whether liquid droplets condense by homoge- <br />neous nucleation and immediately freeze, also <br />by homogeneous nucleation. In any case, the <br />final product is a cloud of very small ice crys- <br />tals, each much less than I ILm in maximum di- <br />mension. <br />Although homogeneous nucleation of the ice <br />phase can be produced by a large number of <br />chilling agents, dry ice remains the most popu- <br />lar. Apart from a few cases in which dry ice has <br />been elevated from the ground by either teth- <br />ered or free-floating balloons, most applications <br />of dry ice have involved dropping pellets from <br />airplanes. In some projects the dry ice has been <br />crushed before being loaded into the aircraft. <br />Other projects have utilized on-board dry ice <br />crushers. The disadvantage of the former <br />method is loss of dry ice by sublimation. During <br />the crushing, sieving, and subsequent storage, <br />both prior to flight and in hoppers on the air- <br />craft, more than half of the dry ice originally <br />provided may sublime away before any opera- <br />tions are conducted. The latter method poses <br />the requirement of carrying additional equip- <br />ment on board the aircraft, namely, the dry ice <br />crusher. Another method, which has been used <br />in the Soviet Union, is to transform liquid CO2 <br />into dry ice on board the aircraft. This method <br />produces a very fine "snow" or "dust" of dry <br />ice. <br />The effectiveness of dry ice is usually ex- <br />pressed as the number of ice crystals produced <br />per gram of dry ice sublimed. It appears that the <br />effectiveness of small pellets with low fall <br />speeds is somewhat greater than that of large <br />pellets. It appears too that the number of crys- <br />tals produced is reduced at ambient tempera- <br />turesjust below ooc. With these caveats, experi- <br />mental data indicate the effectiveness of dry ice <br />to be in the range of 1012 to 1013 ice crystals per <br /> <br />gram. A common technique in dry ice seeding is <br />to drop the dry ice from, for example, the <br />-120C level, using pellets sized so that they will <br />compl<~tely sublime away near the - 50C level. <br />This procedure requires the dropping of pellets <br />1.5 to 2 cm in diameter. In view of the very large <br />numbers of ice crystals produced per gram of <br />dry ic<~ used, it is possible to affect large vol- <br />umes of cloud by dropping modest quantities of <br />dry ic<~, for example, 100 kg per flight. There- <br />fore, dry ice seeding missions can be carried out <br />by small single-engined aircraft. <br /> <br />C. TYPES OF SILVER IODIDE GENERATORS <br /> <br />We have already referred to the ice nucleating <br />properties of silver iodide (AgI) crystals. Unlike <br />natural ice nuclei, most of which are operative <br />only at temperatures below -15 to - 20oC, AgI <br />particles can nucleate ice at temperatures as <br />high as -4 to -50C. The most common form of <br />AgI is a yellow hexagonal crystal with a density <br />of 5.68 g/cm3 . In the hexagonal crystal the silver <br />and iodide ions assume positions analogous to <br />those of the oxygen atoms in an ice lattice, and <br />the spacings are very similar. The separation be- <br />tween the oxygen atoms in the c-plane of an ice <br />lattice is 0.452 nm, and the corresponding spac- <br />ing of silver and iodide ions in the AgI crystal is <br />0.459 nm. There exists a cubic form of AgI, <br />which is also an effective ice nucleant. <br />Any device designed to produce small AgI <br />particles is called a silver iodide generator. Most <br />generators work on the principle of vaporizing <br />AgI and allowing it to solidify upon cooling into <br />small particles. The vaporization of the AgI is <br />sometimes accomplished with electric arcs, but <br />usually with a flame that may be either continu- <br />ous or associated with an explosion. The melting <br />point of AgI is 5520C and its boiling point at a <br />pressure of I atm is 15060C. Typical generators <br />work with flame temperatures around 10000C so <br />that the AgI sublimes or evaporates without ac- <br />tually boiling. It is important that the AgI not be <br />exposed to a reducing atmosphere in the flame <br />for any length of time, lest it decompose into <br />silver and iodine. The tendency to dissociate can <br />be suppressed by use of moderate flame temper- <br />atures, by adding iodine vapor to the flame, and <br />by minimizing the period during which the AgI is <br />exposed to the flame temperature. <br />A very common type of generator uses AgI <br />solutions in a flammable solvent, usually ace- <br />tone. Because AgI is not soluble in acetone, a <br />solubilizing agent or carrier must be used. The <br />most common ones are sodium iodide (NaI), po- <br />