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<br />Severe convective storms have been considered in terms of a <br />simple dichotomy developed by Browning, Chisholm, Marwitz and others, <br />but presented most succinctly by Browning (1978). In this idealiza- <br />tion, one type of storm is the supercell characterized by a large, <br />vigorous, steady updraft so strong that there is insufficient time <br />for precipitation to grow appreciably in its core, and updraft <br />diameter so large that mixing with the environment is minimal. <br />Therefore, one of its distinctive features is a region of weak radar <br />echo that is bounded on its top and all si~es by radar echo of <br />greater intensity. The organized cirulation in this type of storm is <br />thought to provide for an extreme precipitation size-sorting such <br />that the largest particles grow the fastest. For this reason, <br />supercell storms in general are thought to produce exceptionally <br />large hail. At the same time, they are proposed to be inefficient as <br />total precipitation producers because of the updraft strength and its <br />isolation from particles of the size that can effectively collect the <br />cloud droplets and bring the water substance down to earth. Browning <br />and Foote (1976) argued convincingly that the extreme size-sorting in <br />supercells would make hail suppression by seeding difficult if not <br />impossible, and that seeding such storms might even produce more <br />hail. <br /> <br />The second conceptual thunderstorm type is the multicell, which <br />is envisioned to be composed of an organized series of simple convec- <br />tive cells, as first described in The Thunderstorm (Byers and Braham, <br />1949). Each cell has a 30 to 45 min life-cycle, starting with vigor- <br />ous updrafts and no precipitation and ending with downdrafts and the <br /> <br />13 <br />