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<br />8 <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 />I <br />I <br />I <br /> <br />expected size effects for nucleation. Experiments were also performed <br /> <br />with the full polydisperse particle size distributions for comparison. <br /> <br />Comparisons made between cloud chamber experiments and numerical <br /> <br />model simulations were made "equivalent" in the sense that temperature, <br /> <br />pressure, humidity and ascent rate were identical. Cloud condensation <br /> <br />nuclei activity was controlled in the laboratory experiments and <br /> <br />specified in the model simulations. Items which were not simulated were <br /> <br />considered to be of secondary importance in these experiments. They <br /> <br />include turbulent mixing, interactions with precipitation size <br />particles, radiation effects, and electric field and particle charging <br /> <br />effects. Additionally, some aspects related to the long term residence <br /> <br />of ice nuclei in the atmosphere, namely photodeactivation and potential <br /> <br />reactivation following evaporation, were not studied. <br /> <br />Comparative field experimental data were obtained from <br /> <br />tracer/seeding experiments conducted in North Dakota cumulus clouds <br /> <br />(Stith et al., 1990). These experiments used AgI-AgCl aerosols. <br /> <br />Specific experimental plans are outlined in chapter 4, and are <br />discussed further in Chapter 5. <br /> <br />1.4 Expected Utility of Results <br /> <br /> <br />The results of this research should have a number of applications, <br /> <br /> <br />as enumerated here. <br /> <br />1. It is important to compare laboratory experiments and computer <br /> <br />model simulations and to evaluate how well the results can be <br /> <br />extrapolated to real atmospheric situations. The results from <br /> <br />this work should provide a more valid description of the early <br />