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<br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br /> <br />Utah to the northwest, brought dry air into the area and ended this second storm period. <br />Each of the two upper level troughs had an accompanying surface cold front. By 1700 MST <br />on 7 February one surface low was located in northern California with a cold front arcing <br />southeastward into Kevada then back southwest\vard through southern California and offshore. The <br />trough to the north began pushing an east-west oriented cold front southward, so that it was <br />positioned across southern OreQ"on and Idaho bv 1700 on 7 Februarv. Bv 0500 on 8 Februarv the <br />- . - .. .. <br /> <br />southern system had developed a low over central ),jevada with its cold front crossing the southwest <br />comer of Ctah_ and extending southward along the western border of Arizona. The northern cold <br />front stalled but an elongated surtace low developed across northern Utah and Colorado, merging <br />with the low over ~eYada. This complex low pressure area moved east\vard directly across Utah, so <br />that by 1700 on 8 February it \vas on the Utah-Colorado border. A cold front from the southern low <br />pressure area may have passed the research area about midmorning on 8 February. <br />The seeding experiment times and the evolution of the storm over the Wasatch Plateau are <br />sho\\n in the data from RRS plotted in Figs. 9 and 10. The arrival of moist air is seen in the rapid <br />increase in both vapor and liquid depth beginning at 0500 on 7 February. Over the first 10 hours of <br />the storm liquid depths often exceeded 1 mm. This occurred during a period of cloud seeding \vith <br />AgI from a set of four valley-based generators. Icing at RRS was consistent and vvinds at mountain <br />top level were 230 - 2400 and increased in speed to about 9 m s-: by 1200. The cloud field during one <br />research aircraft night from 1045 to 1410 is shown in Fig. 11, indicating the research area remained <br />under a region of relatively warm-topped clouds with a colder cloud shield located to the south. This <br />indicates that the early part of the storm lacked a seeder cloud system, and likely accounts for the <br />high SL \V amounts in the feeder cloud. <br />A slight suggestion of the first short wave passage is seen in Fig. 9 at about 2200 when the <br />\\ ind speed increased markedly, the temperature dropped about 2 ~ and "vind direction veered briefly <br />to about 2600. This was preceded by a well defined maximum in SL W depth and the highest icing <br />rates of the storm. Supercooled liquid \\c'ater depths were periodically high throughout the night of <br />7 February and into the early morning of8 February. The periodicity noted in Figs. 9 and 10 appears <br />to be on a scale of 2-3 hours between maxima, and suggests persistent mesoscale influences. The <br />,,\ind pattern. particularly speed, on 8 February also showed relatively large fluctuations, indicative <br /> <br />17 <br />