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<br />I <br /> <br />47 <br /> <br />I <br /> <br />4.1.1 Deposition Nucleation Experiments <br /> <br />I <br /> <br />The approach to the deposition studies was to perform continuous <br /> <br />expansions to water saturation in the dynamic chamber at a slow ascent <br /> <br />I <br /> <br />rate, to cover the range of humidities between ice saturation and water <br /> <br />I <br /> <br />saturation for temperatures between -50C and -20oC. In this way. <br /> <br />nucleation of freezing of the liquid phase was limited from influencing <br /> <br />I <br /> <br />the results. A thermodynamic path for such an expansion is demonstrated <br /> <br />in Fig. 4.2. The measured cumulative ice crystal flux settling from the <br /> <br />I <br /> <br />cloud could be related to a given temperature and percent ice <br /> <br />I <br /> <br />supersaturation (S.). S. was determined from the humidity measurements, <br />1. 1. <br /> <br />with verification provided by the observed thermodynamic cloud point. <br /> <br />I <br /> <br />This approach assumes that once the critical supersaturation is <br /> <br />exceeded, nucleation occurs instantaneously; and the time response of <br /> <br />I <br /> <br />the experiment is limited by ice crystal growth and fallout. Only <br /> <br />Anderson and Hallett (1976) have noted a finite delay before the onset <br /> <br />I <br /> <br />of nucleation at some defined temperature and supersaturation. Edwards <br /> <br />I <br /> <br />and Evans (1960) and Schaller and Fukuta (1979) did not find this delay <br /> <br />and neither study observed any nucleation to occur after initial ice <br /> <br />I <br /> <br />formation. <br /> <br />To evaluate such potential effects in the dynamic cloud <br /> <br />chamber, one couid conduct intermittent expansion experiments in which <br /> <br />I <br /> <br />a set of conditions are established and held to measure the nucleation <br /> <br />I <br />I <br /> <br />rate and the ultimate number of ice crystals that formed, followed by <br /> <br />another brief expansion to produce a higher value of Si' at a slightly <br /> <br />colder temperature. This has not been done due to the additional time <br /> <br />that would be needed to implement the special coolant control procedure <br /> <br />I <br /> <br />required. <br /> <br />I <br /> <br />I <br />