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<br />JUNE 1990 <br /> <br />TERRY DESHLER AND DAVID W. REYNOLDS <br /> <br />483 <br /> <br />182500 UTe <br /> <br />t ! J ] ,l ! ~ !.. r !- ~ r ~ ! r J J ! .If r J ! f t r } !. ~ r ~} ! ! ! ) ! ,r !. j' ! r ! J I r !. I .l ,I. r ! r ), j ~ J ! r ! ! t t <br />Wi illll II/III II1I JlII/III )1111 11111111//11111 IIIIII1I1IIIIII jlllllllllJ I JIIIIIIIIIIIIIIIIIII jllllll/III/lll JIIIIIIII!)I 1111111111111111/111 i/II/IIIII /1/1111111111 JlJ 111//11111 I ImlllIIll1 IIIIIIllIIlllllllllll1 1111/ I/III/IIII/II//IIIIII 1//)/1 JI/IIIII/IIII JlJllJiJ I <br />r ! !~ J !~ r f ~ ~ ~ I J ! ), !' j ! ~ ~ t ), r .It .l !. ,r ! H. ! f !. !I j' J } ! ! !. !. !, ! ,~ ,L ,~ r ) ! ,I J .r f t ,~ ~ ). ! ! ! <br /> <br />183637 UTe 2D-C 1--1 0,8 mm <br /> <br />~ r ~ ~ I fi. 1(' \. " i' ~ j:- i j' ! '" f' ,_ V I, r L ~~~ l" , i l.-,.. f- i rr...... !J ~ i- 'LL. <br /> <br />I . I I I ,. ., it'- " i.. ,. I " I I I 1', " I I~" ,- <br />2D-P I-----l 6.4 mm <br /> <br />. Jt I J JIIII J IIIJIII J}JIIIJ~ H filii I I j' II IJ~I!Hj IIIIII J IJJ 1 tlHi/11 JJJH It~jll HI j Illl!' II IlfH II I J ilJ I I 11111fl} IIHrJI I if IJ Hili 111l- It IIIIJ IJIIIHI j, jH~iJ Illfl If J IHJIIIt} IIIIII I ijT~ II JJIHJJ JtH <br />!~ I!' rl, ~ h ,j ,lif r f j ~ ! ,IGJ-f ,l.--l ~ ,i.J/f j.- f' ,f f J.} J~ j~ r j l !. f !_ ~ jeGt ,~ <br /> <br />FIG. 3. Images from the 2D-C and 2D-P showing water drops and frozen drops with protruding needles. <br />The center row of images in each set is from the 2D-P. <br /> <br />J- <br />, <br /> <br />Images indicated that the particles in the seedline <br />were primarily graupel and plates, while outside the <br />seeded plume branched crystals and aggregates were <br />observed. Within the seedline the crystal habits are <br />consistent with nucleation and growth at temperatures <br />between -8 and -l2OC, where thick columns and <br />plates are expected (Magono and Lee 1966). These <br />. compact crystal-types rime efficiently and graupel could <br />easily result (Heymsfield 1986). In contrast, outside <br />the seedline branched crystals and aggregates were ob- <br />served, which are consistent with nucleation and <br />growth near the top of the cloud, -IS oc. <br />The cloud conditions and ice crystal types observed <br />during these final penetrations are not similar to cases <br />when ice multiplication was observed during the SCPP <br />(Deshler et al. 1990), and it is unlikely that an ice <br />multiplication mechanism would confine itself to the <br />seedline. The increases in ICC observed during the <br />seedline penetrations shown in Fig. 4 are also not be- <br />lieved to result from aircraft-produced ice particles <br />(APIPS). During the SCPP several specific experiments <br />were conducted to test for APIPS from the seeder air- <br />craft and no evidence was found (Gordon and Marwitz <br />1986), although in other experiments the research air- <br />craft was found to cause APIPS in 2 out of 37 pene- <br />trations (Marwitz et al. 1986). During the first II pen- <br />etrations of the seedline on this day the research aircraft <br />made repeated penetrations of a point drifting with the <br />wind. If the aircraft was producing ice particles they <br />should have been observed during these penetrations <br />since the aircraft repeatedly returned to the same point, <br />yet no unusual increases in ICC were observed until <br />the last 2 of these II penetrations when the aircraft <br />had climbed. However, definite increases in ICC at the <br />seedline were observed during the final five penetrations <br />(all shown in Fig. 4), and these were made at different <br />points along the line. The aircraft flew a "Z" pattern, <br /> <br />advecting with the seedline, but moving from the center <br />of the seedline to the north end. Thus these particles <br />could not have been nucleated by the research aircraft. <br />The seeding material was released in the upwind edge <br />of an orographic cloud with radar reflectivities of 15- <br />20 dBZ. Although there was evidence of ice generation <br />near 5 km, and subsequent enhancement of reflectivity <br />as the particles fell through the cloud, the echo region <br />was generally below 5 km. The seedline remained with <br />this same level of background echo throughout the 92 <br />min of sampling and there were no changes in reflec- <br />tivity that could be attributed to seeding. This is typical <br />for this type of cloud. Deshler et al. (1990) found in <br />similar experiments that only 4% of the clouds had a <br />background echo low enough for the radar to be sen- <br />sitive to seeding effects. <br />A schematic of the cloud and barrier in two dimen- <br />sions is shown in Fig. 5. The seeding location, the X- <br />Zlocation of the research aircraft during seedline pen- <br />etrations, and the expected envelope of AgI IN, based <br />on the detection ofIN at 64 min and assuming a vertical <br />dispersion of 0.1 m S-I, are also shown. According to <br />this calculation the research aircraft was generally below <br />the IN for the first hour. Note that the ascent of the <br />seeding material between 61 and 92 min, 0.2 m S-I, <br />parallels the slope of the barrier. Also shown in Fig. 5 <br />are predictions for the trajectories of ice crystals nu- <br />cleated after delays of 5, IS, 30 and 45 min, from a <br />targeting model used by the SCPP (Rauber et al. 1988). <br />Although for this case the direction of the model winds <br />and the aircraft measured winds are in good agreement, <br />the model winds are slower by 4 m S-I. This causes <br />the disagreement between the predicted seedline po- <br />sition and the aircraft determined seedline position at, <br />for example, 60 min. <br />The model predictions of fallout give an average ad- <br />vection of seeding material to the surface of 2330 at <br />