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<br />1162 <br /> <br />JOURNAL OF APPLIED METEOROLOGY <br /> <br />VOLUME 27 <br /> <br />physical observations completely verified earlier sta- <br />tistical findings based on a large number of storms. Yet <br />there are no apparent inconsistencies between the <br />physical and statistical approaches. The January 1985 <br />seeding was effective in some but not all cases. The <br />successful seeding was done with Main Ridge temper- <br />atures of -90C or colder, moderate to strong westerly <br />flow, warm cloud tops, and SL W present. This is in <br />agreement with earlier statistical suggestions and cur- <br />rent physical understanding. <br /> <br />6. Crosswind widths of the seeded zones <br /> <br />It is of interest to document the widths of the AgI <br />seeding plumes and the associated ice particle plumes <br />over the BR T A, because such information can suggest <br />the appropriate crosswind distance for placement of <br />AgI generators for any future seeding programs with <br />terrain and clouds similar to those at the Bridger Range. <br />The width of the ice particle plumes caused by AgI <br />seeding were determined as described for the enhanced <br />IPC zone in section 3. These were estimated by ex- <br />amination of buffer- by-buffer IPC measurements from <br />the 2D-C probe. Ice particle plumes clearly caused by <br />seeding were apparent on the 10 and 15 Jan missions. <br />The widths of these plumes are shown in Table 2 for <br />each pass except for the last three of 15 Jan, which had <br />decreased IPC due to earlier cessation of seeding. The <br />mean IPC is also noted. Supporting wind and stability <br />data can be found in Table 3. <br />The mean plume widths at the lowest sampling level <br /> <br />TABLE 2. Summary of ice particle plume widths and mean ice <br />particle concentrations (IPC) for N-S passes with enhanced IPC due <br />to seeding. <br /> <br />Date <br />(1985) <br /> <br />Altitude Width Mean IPC <br />(km) (km) (L-') <br />2.7 2.1 12 <br />2.7 5.8 11 <br />2.7 4.9 8 <br />2.7 8.1 3 <br />3.0 3.5 9 <br />3.0 3.3 14 <br />2.85 5.2 17 <br />2.85 3.3 15 <br />2.7 5.3 15 <br />2.7 10.7 7 <br />3.0 4.1 6 <br />3.0 2.0 7 <br />2.85 7.7 18 <br />2.85 10.6 14 <br />2.7 7.3 19 <br />2.7 9.1 12 <br />2.7 8.6 14 <br />2.7 9.1 13 <br />2.7 9.0 21 <br />2.7 7.3 21 <br /> <br />10 Jan <br /> <br />15 Jan <br />(a.m.) <br /> <br />15 Jan <br />(p.m.) <br /> <br />(2.7 km) were 5.2 km for 10 Jan, 8.0 km for the morn- <br />ing of 15 Jan, and 8.4 km for the afternoon of 15 Jan. <br />Comparison with Table 3 shows that the mean ice par- <br />ticle plume was narrower than the mean AgI plume in <br />the 10 Jan case, presumably due to the limited cross- <br />wind extent ofSLW. Table 2 also shows that the plume <br />was narrower at 3.0 km than at 2.7 km on both the 15 <br />Jan missions. Mean ice particle concentrations were <br />remarkedly consistent, ranging only from 3 to 21 L -1, <br />with only two values below 7 L -1. Table 3 lists AgI <br />plume widths estimated with the acoustical counter <br />for pairs of2.7 km passes along the N-S sampling line <br />over the BRTA. Also listed are wind and stability in- <br />formation, both upwind of the Bridger Range and over <br />the BR T A. The mean concentration of AgI was esti- <br />mated by dividing the mean adjusted total counts by <br />the plume width. In this case the total counts per pass <br />were multiplied by ten to adjust for chamber losses, as <br />suggested by Langer (1973). The mean concentration <br />is effective at -200C, the acoustical counter cloud <br />chamber temperature. Concentrations would be about <br />an order of magnitude less at -1 OOC but only a factor <br />of two less at -120C, according to the AgI generator <br />calibration of Garvey (1975). Comparison of 10 Jan <br />IPC values in Table 2 with corresponding AgI concen- <br />tration values in Table 3, adjusted downward by the <br />factor of two for the prevailing temperature of -120C, <br />suggests that a small fraction of the available AgI nu- <br />cleated ice crystals. This may be due to the long time <br />dependence of contact nucleation, discussed by Demott <br />et al. (1983), for the low water content cloud found <br />on 10 Jan, Agreement between IPCs and ice nucleus <br />concentrations was much better on the wetter 15 Jan <br />missions if Table 3 values are reduced by a factor of <br />ten for the warmer prevailing temperatures. <br />Excluding the apparently meandering plumes in the <br />very stable atmosphere of 19 Jan, AgI plume width <br />estimates ranged from about 2 to 8 km. The mean <br />value for the 12 estimates in 5.2 km, which compares <br />with a mean of7.3 km for all 2. 7 km ice particle plumes <br />in Table 2. Tables 2 and 3 both suggest that the seeded <br />zone at 2.7 km over the BRTA was infrequently less <br />than 4.7 km wide. The range of conditions samples <br />was somewhat limited, since five of the six missions <br />had a moderately stable atmosphere over the BRTA. <br />Wind speeds there varied from 6 to 15 m S-I and di- <br />rections from 2680 to 2990. However, as shown by SH <br />and by Super (1986), these were typical values during <br />the BRE. <br />The BRE used two AgI generators with about a 6.4 <br />km crosswind separation. The present work suggests <br />that another generator between those two would have <br />been advantageous, especially since time-averaged <br />plumes tend to have Gaussian distributions with con- <br />centrations tailing off toward each edge. Although this <br />was suspected from AgI plume tracing during the BRE, <br />resources did not permit operation of a third seeding <br />site. <br /> <br />I <br />I <br />'. <br />! <br /> <br />/' <br /> <br />'~ <br />