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<br />. <br /> <br />23 <br /> <br />. <br /> <br />hygrometer cylinder, a thermometer, with O.lOC accuracy, indicated the dew <br />point temperature of the fog. From the air temperaure in both the <br />suspension chamber and the sealed cylinder at the moment of fog <br />condensation, the Clausius - Clapyron equation gave the vapor density in <br />both places, and the difference between the densities was the liquid water <br />content of the fog. <br />A hot-wire anemometer, which replaced the pitot tube assembly, greatly <br />improved the measurement of the updraft speed near the crystal in the <br />suspension tunnel. A small sensor placed in the center of the tunnel near the <br />ice crystal provided a more accurate setting for the anemometer than that for <br />the pitot tube assembly since the flow speed was not uniform within the <br />tunnel. <br />The improvements in the experimental techniques increased the <br />accuracy of the determined data set. Furthermore, the longer growth periods <br />attained in this study made the ice crystal growth data more useful at <br />temperatures between -3 and -210C. The data set consists of ice crystal mass <br />and a-axial length after 10, 13, 16 and 19 minutes, c-axiallength after 10, 13 <br />and 19 minutes and terminal fall speed after 7, 13 and 19 minutes of growth. <br />A few problems remained including irregular shape and thin plates, <br />which made the measurements of the dimensions, particularly the c-axis, <br />difficult. However, because of the improvements made in the study and the <br />sound techniques borrowed from Kowa (1981), the problems are <br />comparatively insignificant. <br /> <br />t <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />Takahashi and Fukuta ( to be published) <br />The investigators of this study inherited the techniques and equipment <br />from the study of Gong and Fukuta (1985) and Kowa (1981), but made a few <br /> <br />. <br />