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<br />- 114 - <br /> <br />diameter with an ave~age size of about 3000 ~m, Larger c~ystals than this <br />were observed on the ground, <br />Both air and g~ound observations indicated that these crystals may be <br />readily broken up in the air. <br />4.2,13 8ide Planes (81), Combinations of 8ide Planes, Bullets and Columns <br />(83) and Radiating Assemblage of Plates (P7a) <br />According to Ono (1970), side planes (81) form at temperatures below <br />-220C. Magono and Lee (1966) indicate that side planes (81) grow at <br />temperatures between -20 to -25oC and combinations of side plates, bullets, <br />and columns (83) at temperatures below -250C. The growth region for <br />radiating assemblage of plates is not mentioned by these workers. <br />Our aircraft observations confirmed that all these crystal types grew <br />at temperatures below -l80C and at water saturated conditions. Preliminary <br /> <br />results from ground measurements in this study indicate that cloud tops could <br /> <br />have been warmer than -250C when combinations of side plates, bullets, and <br /> <br />columns (83) were observed on the ground. Taken into account when considering <br /> <br />temperature of the cloud tops was the origin and trajectory of these particles, <br /> <br />Aircraft observations indicated that usually these crystal types occurred as <br /> <br />single crystals but occasionally they were found in aggregates. At the ground <br /> <br />these crystals were usually aggregated. <br />Side planes (81) were numerous both in the air and on the ground, They <br /> <br />were the most common cold region crystal to reach the surface. Radiating <br /> <br />assemblages of plates were also commonly observed at ground level. Observed <br /> <br />more commonly in the air than on the ground, but least common of all, was the <br /> <br />combination of side planes, bullets, and columns. <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 />