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<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 />37 <br /> <br />and FORTRAN 77 programs and a statistical graphics package, after data <br /> <br />are converted to compatible ASCII formats and transfered through one of <br /> <br />the CSU CYBER 206' s. A new data system based about a single 386 PC <br /> <br />machine will soon replace the old data system (DeMott and Rogers, <br /> <br />1990). Improvements in ice detection systems will also be made. <br /> <br />3.2 Isothermal Cloud Chamber <br />The CSU isothermal cloud chamber (ICC) has been described <br />previously by Garvey (1975), and DeMott et al. (1983). The chamber is a <br />closed cylindrical double shell with an inner shell of 0.64 em <br />aluminum, 1.37 m in diameter and 1.52 m high. The outer shell of 10 <br /> <br />gage steel is 1. 68 m in diameter, and the annular space between the <br /> <br /> <br />shells is filled with polyurethane insulation. Cooling is achieved by <br /> <br /> <br />a two-phase Freon flow in a system of 1.5 cm tubes welded to the <br /> <br /> <br />outside of the inner shell at 15 em spacings. These features were <br /> <br />designed to maintain wall temperature within +/- O.l'C around the <br /> <br />chamber walls. The inner shell of the chamber is fitted with a black <br /> <br /> <br />velvet liner about. l5 cm from the wa~ls. Originally installed to <br /> <br /> <br />minimize frost accumulation and shattering, the liner has proved <br /> <br /> <br />important in maintaining an experimental volume with an acceptable <br /> <br />cloud density gradient. <br />The cloud is introduced using the system shown schematically in <br /> <br />Figure 3.7, from DeMott et al. (1983). Cloud droplets are generated <br /> <br />continuously by the atomization of distilled water with an ultrasonic <br /> <br />humidifier (Monaghan 670). They are then mixed with cold air and <br /> <br />allowed to equilibrate with the chamber while rising through a standing <br /> <br />tube in its center. By varying dilution airflo~, the liquid water <br />