Laserfiche WebLink
<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 />13 <br /> <br />Surface observations of ice nuclei concentrations at Climax were also <br />reported by Hindman (1967). Hindman investigated the relationship <br />between ice nuclei concentrations at the Climax High Altitude <br />Observatory and ice crystal concentrations in snowfall during two seeded <br />and two non-seeded storm events. After making several assumptions <br />concerning the large scale and microstructure of the storms analyzed, he <br />concluded that concentrations of ice nuclei and ice crystals were <br />similar in the non-seeded cases but differed by an order of magnitude in <br /> <br />the seeded cases (ice nuclei higher). Hindman also presented limited <br /> <br />data on the crystal types and accretion characteristics of precipitation <br /> <br />during these two storm events. More deta~led summaries of crystal <br /> <br />habits, sizes and accretion characteristics as well as ice nuclei <br /> <br /> <br />observations during the Climax experiments were presented by Grant <br /> <br />(1965), Chappell (1967), and Chappell (1970) and Vardiman (1972). <br /> <br /> <br />Vardiman (1972, 1978) also discussed fragmentation as a possible means <br /> <br /> <br />of crystal concentration enhancement in Climax cloud systems. <br /> <br /> <br />Radar observations of cloud systems during the Climax experiment <br /> <br /> <br />were reported by Furman (1967). Furman examined the echo <br /> <br /> <br />characteristics of four spring storms with horizontally and vertically <br /> <br /> <br />scanning 3 cm radars. He determined that mean cloud tops over the <br /> <br /> <br />Climax region during these storms varied from 450-SS0 mb, although cloud <br /> <br /> <br />tops occasionally reached the 3S0 mb level. Furman's analysis implied <br /> <br /> <br />that the most intense precipitation (strongest echoes) were consistently <br /> <br /> <br />located in the vicinity of ridgetop and that propagation of the echo <br /> <br /> <br />pattern closely followed the SOO mb velocity vector. His work primarily <br /> <br /> <br />emphasized convective periods which could be most readily observed with <br /> <br />the available radar. <br /> <br />