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<br />5. Twenty-five Bureau of Reclamation PROBE micronet stations which <br />measured winds, temperature, pressure, relative humidity, and <br />precipitation <br /> <br />6. Rawinsonde sites, one 60 km upwind, the other 30 km downwind of <br />the barr'i er <br /> <br />7. Satellite images from the GOES West satellite and NMC synoptic data <br />3.1.2.2 Closed data set <br /> <br />A similar COSE data set is available for the closed orographic experiment. The <br />initial flow conditions and soundings will be provided in the same format as the <br />open case from the three-dimensional model. <br /> <br />3.2 Sensitivity tests <br /> <br />Any of the open data sets may be used for model sensitivity cases; however in <br />order to facilitate comparisons among models four cases are proposed for speci- <br />fic tests. <br /> <br />3.2.1 Fluid dynamics <br />3.2.1.1 Initialization <br /> <br />A. GATE 226 - August 14, 1974 <br /> <br />GATE experiment operations on August 14, 1974 were specifically designed to <br />study the structure of the boundary layer in relation to a line of towering <br />cumulus over the tropical ocean. Hence this case which was selected for the <br />open data set in experiment 3.1.1.1.1 is appropriate for boundary layer sen- <br />sitivity analyses also. Please refer to section 3.1.1.1.1 for a description of <br />this case. <br /> <br />This case provides relatively simple, weakly forced conditions in which complete <br />aircraft observations of low level convergence are available. Thus it offers <br />a good opportunity for sensitivity tests of convergence, thermal, or moisture <br />perturbation and combinations of the two mechanisms. <br /> <br />B. CCOPE - June 20, 1981 <br /> <br />Numerical studies of the evolution of convection under conditions of weak large <br />scale forcing have been conducted on this case by Smolarkiewicz and Clark <br />(1984). This case was selected for model initialization experiments because <br />convection that developed early in the day w,as driven by local heating without <br />large scale forcing. Cumulus clouds developed in the morning and were studied <br />by two cloud physics ai rcraft as described by Fankhausl~r et al. (1983). Cloud <br />bases ranged from 1.9 to 2.5 km. Cloud tops reached 6.0 km by early afternoon. <br />Time lapse cloud photographs from 0700 to 1300 LST indicated cumulus humilis and <br />cumulus congestus clouds with diameters of -5 km and durations -20 min. Later <br />in the day larger clouds moved into the network. <br /> <br />19. <br />