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<br />.. .~ <br /> <br />8.20. Heimbach, J. A., and W. D. Hall, 1996: Observations and modeling of va /ley-released silver <br />iodide seeding over the Wasatch Plateau. 13th Conference on Planned and Inadvertent Weather <br />Modification, Atlanta, GA, American Meteorological Society, 31-37. <br /> <br />. . <br /> <br />ABSTRACT <br /> <br />This. paper examines the transport of surface-released silver iodide (AgI) over the Wasatch Plateau of <br />central Utah during inversion conditions. Other case studies of transport have been reported for the <br />Wasatch Plateau. For example, Super and Huggins describe targeting of valley- and canyon-released AgI <br />in an analysis of surface observations (1992a) and aircraft observations (1992b) from the 1989-90 field <br />season. Surface silver-in-snow and real-time ice nucleus (IN) measurements indicated that AgI was. <br />transported up the canyon 'over the Wasatch Plateau but in limited amounts. Co-released sulfur <br />hexafluoride SF 6 was detected by the aircraft for one of five flights. These two papers. highlighted the <br />difficulty in targeting seeding material. Heimbach and Hall (1994) modeled'various release <br />_configurations in a case which had neutral stability and no imbedded convection. They found transport of <br />seeding material over the Plateau also demonstrated that downwind depletion of liquid water (L W) was at <br />least in part due to subsidence warming within a gravity wave pattern. Holroyd et al. (1995) reported on <br />the analysis of the 21 February 1994 experiment which had weak surface winds, light snowfall and weak <br />convection in thin orographic clouds over the Plateau. On this date AgI and SF 6 were co-released from a <br />site part of the way up the windward side of the Plateau. A microphysical seeding signal was associated <br />with the IN plume both at the surface and aloft. Modeling results of transport were reasonably close to <br />observations for this case. Bruintjes et al. (1995) applied the Clark model to three cases from the 1987 <br />Arizona/NOAA Cooperative program. Each of these had a single point-source ofSF6. Results from field <br />observations and the modelled them to conclude that the transport and diffusion of seeding material are <br />dependent upon the flow and stability conditions around the valley release site, and gravity waves <br />stimulated by the upwind terrain. <br /> <br />~ <br /> <br />DISCUSSION <br /> <br />The transport of AgI released from three valley sites was examined for an experiment conducted on <br />7 February 1994. Sulfur hexafluoride was also released on this date from the mouth of a canyon located <br />on the windward side of the Plateau. The observations indicated transport of the AgI over the Plateau <br />mostly within a shallow layer in spite of being released in a stable surface layer with weak and sometimes <br />easterly winds. <br /> <br />Atthe RRS and TAR site, concentrations of 100 in vI, effective at -20 oC, were co~monly sampled. The <br />temperatures at this sites were approximately -6 oC. The IN effectiveness of the generators and solution <br />used in the valley is 2.5 orders of magnitude less for -6 oC (DeMott et al., 1995), giving an effective <br />concentration of 0.24 IN L-1. There were, however, periods having concentrations of several thousand per <br />liter effective at -20oC suggesting concentrations on the order of 5(L -1. No IN or SF 6 plumes were <br />detected over the W track. The only significant IN plume detected by the aircraft was over the E trackin <br />the vicinity of the TAR site at 3.5 km MSL(minimum IFR elevation). For the acoustic IN detector, <br />indicated spread of an IN encounter is due to actual spread plus a temporal component from mixing within <br />the cloud chamber (Heimbach et al., 1977). For this reason, estimating the peak concentration of IN at a <br />point is risky for aircraft sampling. Adjusting for cloud chamber mixing, the maximum concentration of <br />IN was less than 20 L.1 effective at -20 oC. The temperature at this level was -8 oC implying the <br />maximum concentration of effective IN was less than 1.5 L -1. The IN targeted zones of supercooled L W <br />over at least some portions of the Plateau, though indications are that this was in a very shallow layer . <br /> <br />" I. <br /> <br />70 <br />