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<br />utilize the NCAR Queen Air over the San Juan Mountains. Based on the results of <br />Elliott et al. (1974) and Marwitz (1974) the decision was made to conduct an exten- <br />sive investigation over the San Juan Mountains of the transport, diffusion and <br />cloud physics processes. It was apparent from the preliminary results from 1973 <br />and 1974 that the airborne results should be placed in the context of the time <br />dependent storm period. Two quite fortunate advances in aircraft instrumentation <br />made this effort most attractive in 1975. First, the NCAR Queen Air was equipped <br />with an inertial navigation system during 1975 and, secondly, the Wyoming Oueen <br />Air was equipped with a Doppler navi.gation system for measuring horizontal winds <br />and an extremely reliable and rather complete cloud physics instrumentation package. <br />This package has made it possible to obtain the kind of reliable and complete <br />cloud physics measurements needed in order to assess the seeding potential of <br />these storms. <br />, The two aircraft were flown OVE!r the San Juan Mountains for 45 hours in 1975 <br />and ~ total of 60 hours during the three years. It is estimated that there was <br />a precipitating cloud over the San Juans during at least 50 of the 60 hours. <br />During the other 10 hours a cloud was either in the process of forming or had <br />recently dissipated. Twelve separate storms were flown in the three years. <br /> <br />IV. Present Status and Preliminary Results <br /> <br />A preliminary synthesis of each of the storm periods has been completed. <br />The data from the NCAR Queen Air fat' the March 1975 storms has been delayed due <br />to software development and excessively long computer turn-around time. The <br />Wyoming Queen Air data has only become available at the time of this writing and <br />an indepth analysis is just beginning. Our present impressions of the cloud <br />processes are primarily based upon data a"ITailable to the onboard scientists who <br />monitored the realtime computer presentations. <br />Based on detailed analysis of the serial rawinsonde data obtained at Durango, <br />a typical storm sequence is presented in :Figure 1. Figure 1 is a vertical-time <br />cross section of equivalent potential temperature (8e), cloud base and cloud top <br />boundaries, region of conditional thermodynamic instability (a8e/aZ < 0) and level <br />below which the winds are not from 1600 through 2800. The typical storm sequence <br />is as follows: <br />28/05 to 28/15: The atmosphere is absolutely stable (a8e/aZ > 0) with clear <br />skies. The surface based nocturnal inversion forms each night and dissipates each <br />morning. The winds below 3.0 kIn are not from 1600 through 2800 due to blocked <br />flow below the mountain in the stable atmosphere. The 500 mb temperatures are <br />well above the -23C specification for seeding. \ <br />28/15 to 28/21: Cold air advection begins above 6 kIn (ae~/dt < 0) and high <br />level clouds form. In this case the clouds are altocumulus but they are typically <br />cirrus. The blocked flow continues below mountain level. <br />28/21 to 28/23: The next occurrence in the sequence is a rapid development <br />and lowering of the cloud base as midlevel moisture arrives. The cloud tops remain <br />high and hence, cold during this period. Our preliminary cloud physics data indi- <br />cate that the concentration of ice crystals is at least 100/t and often exceeds <br />1000/t during this period. The preliminary data also indicate that supercooled <br />water and aircraft icing is quite rare. The winds above mountain top level (3.5 km) <br />begin to increase and the first precipitation begins. The 500 mb temperature <br />decreases significantly during this period but the atmosphere remains stably <br />stratified. Since the winds below 3 km are not from 1600 through 2800 and the <br />turbulence level above 3 kIn is low, any AgI released into this stably stratified <br />cloud cannot possibly seed (or overseed) this cloud. <br /> <br />23 <br /> <br />--- <br />