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<br />2 <br /> <br />The initial results from the SF6 tracing program showed that on very <br />convective days with little wind, the tracer gas was able to be located <br />within about one mile of the release point. When. wind was present the SF6 <br />was found several hundred feet above the ground in convective conditions, <br />but in a comparatively narrow band. When the tracer flowed around a modest <br />(1500 ft high) hill, a clear change in direction of the flow after passing <br />the hill occurred. This may have been due to wind funneling down an upstream <br />valley. All of these results point to the complexities of air flow across <br />mountainous terrain and the need for additional new research and detailed <br />measurements in areas where seeding aerosol releases are to be made. This <br />particularly applies to the need for accurate and continual surface flow <br />measurements. Details of the instrumentation and the flight records and <br />data are given under Section I of this report. <br /> <br />The study of convection over land, below and in stratus clouds was <br />completed and the results published in 1986 in Atmospheric Research, 20, <br />87-100. It shows that the vapor flux from the evaporating snow surface <br />can drive convection and maintain a supercooled water cloud layer without <br />the assistance of heat flux from the surface, or entrainment or radiative <br />cooling at cloud top. Because the saturation vapor pressure over water <br />is higher than that over ice, the base of the supercooled water cloud has <br />a lower limiting height. <br /> <br />When the cloud base is lowered to this height, the air at the bottom <br />of the convective layer is just saturated with respect to ice and the eva- <br />poration of snow stops, as does the vapor-driven convection. This limiting <br />cloud base height varies with snow-surface temperature. . The lower the snow <br />temperature, the higher the cloud base height limit for continued convec- <br />tive transfer from the surface. As an example, if the snow surface tempera- <br />ture is -50C, there could be vapor-driven convection, provided the cloud <br />base height is more than 80 m above the surface. Whereas, if the snow <br />temperature is -lOoC the convection would stop if the cloud base height <br />above the surface became less than 150 m. <br /> <br />Section II. <br /> <br />Precipitation Chemistry and Stable Isotope Proqraa: <br /> <br />The goalS of this work were to measure the trace chemical composition <br />of snow collected at the HALO site and relate this to its stable oxygen <br />isotopic composition and observed ice crystal habit and structure, so that <br />estimates could be made of: (a) the elevation range over which supercooled <br />liquid water is captured by falling ice crystals1 (b) the extent to which <br />AgI and possibly 1n203 are captured by warmer and colder habit ice crystals1 <br />and (c) the extent to which these techniques might be developed for covar- <br />iate analysis of future randomized seeding experiments1 also (d) in <br />cooperation with the SCPP management it was decided that specially-tagged <br />AgI aerosols using Cs1 would be used from aircraft seeding to test the <br />GUIDE model predictions for targeting seeding effects into the HALO site <br />under the fixed target experiment criteria. <br /> <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br /> <br />I <br />I <br />I <br />I <br />I <br />I <br />