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<br />APRIL 1990 <br /> <br />DESHLER, REYNOLDS AND HUGQINS <br /> <br />309 <br /> <br />generally dendrites or dendritic arms. During periods region from the bottom on plot of ICC as a function <br />oflower ICC, such as prior to passage of PI, sheaths, of habit) was diminished. The greatest contribution to <br />needles, and rimed columns predominated. A photo- increased ICe during the PPE of S 1-S3 came from <br />micrograph of ice particles collected at KGV at 1847, particles between 0.3 and 0.5 mm, and particles clas- <br />during the PPE:for PI, is shown in Ff~< 16a. sifj.ect as hexagonal. On the plot of ICC as a function <br />For tl1e seeded experiment an increase in ICC was of habit compare the measurements at 1935 and 1945. <br />observed during the PPE for S2 and S3. S l(arrived The concentration of all habits from graupel up to tiny <br />within the natural precipitation region discuss~d earlier, are identical. The increased ICC at 1945 is solely a <br />and the increased ICC associated with this feature can result of an increase in images classified as hexagonal, <br />be seen. Based on photomicrographs at 1937 (Fig. 16b) a category into which small rimed particles fall. The <br />the predominant snow crystals were dendrites, singly same can be seen comparing the measurements at 1958 <br />and in aggregates, and light to moderately rimM. Based and 2005. Similar features were not observed at other <br />on the radar and aircraft data, S2 was isolated from times during the period shown, nor were they observed <br />surrounding natural echo, and thus provides some in- during the PPE of PI-P3. Thus these measurements <br />sight into the microphysical effects seeding may have are consistent with the photomicrographic observa- <br />on precipitation at the ground. Based on the beginning tions, and with the calculations of Heymsfield ( 1986), <br />and end times of increased ICC at KGV, S2 took: 7 suggesting that seeding produces small heavily rimed <br />min to pass. Thts'is slightly longer than expected based particles. Data from the photomicrographs, shown at <br />on aIm S-I dispersion rate and a speed of 10 ms-I the top of Fig. 15, are consistent with the measurements <br />across the site. The maximum concentration within by the 2D-C. Also at the top of Fig. 15 is precipitation <br />S2 was 13 L - I. Particle sizes from the ground 2D-C rate, from the high resolution gauge located within 10 <br />indicated most particles were between 0.2 and 0.5 mm m o(,the ground 2D-C. Note that increases in precip- <br />with approximately 2 L -[ of particles between 0.5 and itatibn rates of 0.5 to 1.5 mm h -I above background <br />1.0 mm. This was comparable to the concentration of were recorded during the PPE for Sl-S3. Given that <br />particles> 0.4 mm measured with the 2D-P on the these increases occurred over a 7 min period the ad- <br />aircraft at the 39 min pass in S2. Photomicrographs ditional precipitation received from seeding was 0.06 <br />taken at 1947~t the trailing edge of S2 (Fig. 16c) to 0.18 mm. <br />showed that the snowfall was composed of heavily It is also interesting to note that the integrated liquid <br />rimed irregular particles and graupel, with some par- water measured by the vertically pointing radiometer <br />ticles indicative of heavily rimed columns. The particle~', (Fig. 4) showed a marked decrease just prior to the <br />were predominantly 0.5 to 1.0 mm. These particle size's PPE of Sl and S2, with a small recovery before S3 <br />and shapes conform well with calculations by Heyms- arrived. It can only be speculated if seeding contributed <br />field ( 1986 rand Rodi et al. ( 1985). Aggregation was to this decrease in liquid water. <br />not obvious during the passage of S2. This is diffe,rent <br />than the aircraft observations of S2; however, 'the pre- <br />dominant particles observed by the aircraft were small <br />rimed particles and this agrees with the observations <br />at KGV. . <br />A distinct region of higher ICC was observed at KGV <br />at the PPE for S3; although, radar data showed that <br />precipitation from the echo that was observed to be <br />trailing S3 was beginning to affect KGV at this t~me, <br />The first half of this period of high ICC is simjlatin <br />width to S2, indicating a duration of nearly 7 rpin. <br />Photomicrographs taken at 1957 (Fig. 164) inJhe <br />leading edge of S3 showed the snowfall to be; again, <br />heavily rimed, almost spherical, particles of 0.5 to 1.0 <br />mm. Dendrites and dendritic aggregates were observed <br />to be the predominant crystal habits again at 2005. <br />Although not as clear cut as S2, there is an indication <br />that a seeding effect and natural precipitation were oc- <br />cumng III sequence. <br />Considering the bottom two time series plots of ICC <br />in Fig. 15, several interesting characteristics of the <br />seeded plumes can be observed. During the PPE ofS 1- <br />S3 the small but steady concentration of particles be- <br />tween 1 and 10 mm (topmost shaded region on plot <br />ofICC as function of size) and needles (third shaded <br /> <br />'. <br /> <br />4) SUMMARY OF RESULTS <br /> <br />The cloud structure on the 18th was not a simple <br />orographic cloud but more like what Rangno ( 1986) <br />has described as an orographic cloud composed of <br />nimbostratus. The natural precipitation process was <br />dominated by primary nucleation between -150 and <br />-20oC, followed by aggregation and riming as den- <br />drites fell into the lower level liquid water or "feeder" <br />cloud. Within the shallower liquid-cloud the coales- <br />cence, process could be identified, but in discontinuous <br />regions of the cloud, most notably near convection <br />(Mossop 1985). These regions could also be associated <br />with columns and needles possibly formed by primary <br />nucleation in regions of enhanced water supersatura- <br />tions (DeMott et al. 1983) or by the rime-splintering <br />mechanism of Hallett and Mossop (1974). These phe- <br />nomena were documented during experiment I, the <br />placebo case. Although these processes were occurring, <br />they did not glaciate the cloud. Liquid water within <br />these regions remained at 0.1 to 0.3 g m -3. <br />For the seeded regions of this cloud the major results <br />were: <br /> <br />(i) An AgI NH4I NH4Cl04 seeding solution pro- <br />