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<br />556 <br /> <br />IRRIGA nON AND DRAINAGE <br /> <br />1515-1620. High IN concentrations were still found from 1720-1740 along the valley <br />floor with the van. <br />Ice nucleus count rates per minute are equivalent to IN rl for the 10 rl intake flow <br />used with the acoustical counters and the X 10 correction suggested by Langer (1973) <br />for known ice crystal losses. Thus, the DOT IN concentration averaged about 500 rl <br />at the cloud chamber temperature of -200C. In order to estimate the concentration of <br />IN effective at the prevailing DOT air temperature of -40C, the temperature <br />dependence of effectiveness values (ice crystals produced per gram of AgI) for the <br />Utah operational generators (Griffith, et al. 1991) must be considered. Assuming a <br />lower canyon wind speed of 1-4 m S"I, effectiveness values at -60C, -120C and -20oC <br />are about 2 X 1010, 1014 and 3 X 1015, respectively. Extrapolation from-2boC to _60C <br />would reduce the effective IN by 5 orders of magnitude. Calculations with typical <br />SLW condensate production rates indicate that approximately 10-100 IN rl are needed <br />for effective cloud seeding (Yo\lng, 1974). Thus, the 500 rl measured at the DOT at <br />-20oC would provide negligible IN concentrations at -40C. <br /> <br />Silver Iodide Sampling Along the Upwind Highway: Silver iodide was detected all <br />along the highway on all 9 van passes between 1230-1548. The entire 8 km upwind <br />highway appeared to have AgI present throughout the sampling period. This implies <br />that the density of valley AgI generators may be adequate for periods with embedded <br />convection. (However, the density used by the operational program is less than used <br />in the early 1991 experiments). It is speculated that the widespread dispersion was due <br />to a combination of convection within the cloud elements, and mechanical turbulence <br />over the rugged windward slope. <br />The average IN concentrations for each of the 9 passes along the upwind highway <br />ranged from 300-650 rl, effective at -200C. The IN concentration fell to about 50 r1 <br />during the final 1/3 of the last pass as the storm ended. Air temperatures averaged <br />-3.50C on the north end of the upwind highway (elevation 2680 m MSL), and about <br />-5.50C on the south end (2990 m). Negligible effective IN concentrations would result <br />from AgI at these temperatures. The AgI would need to be transported to higher, <br />colder cloud levels to provide adequate IN concentrations. <br /> <br />Table 1. Summary of van measurements of SF6 tracer gas in parts per trillion (ppt). <br /> <br />Mean time Mean SF6 max. SF6 N-S plume Plume center dist. <br />(MSn JIm1L JIm1L width (lan) S. of DOT (lan) <br />1319 40 220 4.0 6.6 <br />1350 30 110 4.4 5.0 <br />1414 20 90 4.2 2.3 <br />1503 100 170 5.5 2.1 <br />1512 35 60 0.8 -0.2 <br />1538 0 0 0.0 N.A. <br /> <br />Tracer Gas Sampling Along the Upwind Highway: Table 1 summarizes surface SF6 <br />observations. Mean SF6 concentrations were in the range 20-100 ppt (by volume) and <br />plume widths were between 4.0-5.5 km prior to 1512. The tracer gas thereafter <br />decreased, presumably because gas release was terminated about an hour earlier. The <br />