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<br />6.40 <br /> <br />7.1 <br /> <br />7.2 <br /> <br />7.3 <br /> <br />7.4 <br /> <br />7.5 <br /> <br />7.6 <br /> <br />A1 <br /> <br />A2 <br /> <br />Comparison of cumulative ice fractions nucleated in cumulus <br />seeding simulations with AgI-AgCl versus AgI-AgCl-4NaCl <br />aerosols. Cases of seeding below 50C cloud base (a) and <br />into cloud at -50C (b) are shown. <br /> <br />Adiabatic cloud model profiles of cloud and thermodynamic <br />quantities in the simulation of the 22 June case. Vertical <br />velocity replaces the supersaturation profile shown in <br />previous figures of this type. A few observations from the <br />real cloud are overlain in repective plots (~). <br /> <br />Time histories of temperature (a) and ice formation (b). <br />-1 <br />Ice is given both as the concentration L and as a <br />fraction of initial aerosol concentrations injected. In <br />(b), observed data are shown (~), from Stith et a1. <br />(1990). <br /> <br />Model-predicted nucleation mode contributions to ice <br />formation in the simulation of the 22 June case (a), and <br />those predicted if seeding had been done with AgI-AgC1- <br />4NaCl aerosols (b). <br /> <br />As in Figure 7.1, for the 28 June case. <br /> <br />Predicted ice concentration versus time (temperature) for <br />28 June cloud. The range of concentrations observed in the <br />upshear cloud region is shown by brackets. <br /> <br />As in Figure 7.3, <br />below cloud base. <br /> <br />but for the 28 June cloud seeded from <br /> <br />Deposition/sorption nucleation active site density (D ) <br />dep <br />on an ice supersaturation-temperature plane, as <br />parameterized in the original model version. <br /> <br />Fractional percentage activity (PCT - F ) by contact- <br />ctf.: <br />freezing nucleation as a function of aerOSOl size and ice <br />supersaturation. <br /> <br />xx <br /> <br />200 <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 />I <br />I <br />I <br /> <br />210 <br /> <br />211 <br /> <br />212 <br /> <br />215 <br /> <br />217 <br /> <br />218 <br /> <br />248 <br /> <br />249 <br /> <br />I <br />I <br />I <br />