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<br />40 <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 />3 <br />content (LWC) can be varied from 0.3 to 3.0 g m without changing the <br />3 <br />droplet size appreciably. Temperature within the 1 m experimental <br /> <br />volume can be maintained to within +/- 0.3.C of the setpoint over a <br /> <br />range from 0 to -25'C. <br /> <br />The cloud density is continuously monitored by means of a <br /> <br />Cambridge Systems dewpoint hygrometer. The technique employed is to <br /> <br />evaporate a cloud sample and measure its dewpoint; the difference <br /> <br />between the saturation mixing ratio corresponding to the dewpoint <br /> <br />temperature and that corresponding to the cloud temperature is taken as <br /> <br />the liquid water content. Temperatures throughout the system are <br /> <br />measured by thermocouples and are recorded continuously. Droplet sizes <br /> <br />have been measured using soot-coated slides with a device patterned <br /> <br />after that of Squires and Gillespie (1952) and using a Particle <br /> <br />Measuring Systems Forward Scattering Spectrometer Probe (FSSP-lOO) <br /> <br />(DeMott et a1., 1983). Mean droplet diameters range between 6 and 9 ~m <br /> <br />on all occasions. Representative mean droplet concentrations are 2100 <br />-3 -3 -3 -3 <br />cm at 0.5 g m and 4300 cm at 1.5 g m LWC. Representative cloud <br /> <br />droplet spectra are shown in Figure 3.8. The cloud simulates a slowly <br /> <br />settling fog or stratus cloud at water saturation, and its quasi- <br /> <br />steady-state nature allows nucleation and ice crystal growth to be <br /> <br />studied as a function of time. <br /> <br />Ice crystals settling from the cloud after injection of artificial <br /> <br />ice nucleating aerosols are collected on microscope slides and are <br /> <br />counted using a cold-box microcope. Slides are sampled from the chamber <br /> <br />periodically until nucleation ceases. The uncertainty in this procedure <br /> <br />is about 30% based on past results. Counts are typically converted to <br /> <br />numbers effective per gram of nucleant dispersed (- Yield), but for <br />