<br />JUNE 1990
<br />
<br />TERRY DESHLER AND DAVID W. REYNOLDS
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<br />483
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<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.
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<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
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