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<br />of a water drop moving through the flow field around a freely <br /> <br />, <br />falling graupel is the system's mixed Froude number. <br /> <br />Third, a <br /> <br />drop-equivalent approach, using the collection efficiencies for <br /> <br />ice spheres derived by Beard and Grover (1974). Fourth, by using <br /> <br />a unity collection efficiency. <br /> <br />It was concluded after canparisons <br /> <br />of calculated with experimental graupel growths that' the mixed <br /> <br />Froude number approach was more accurate than other' methods. A <br /> <br />parameterization was developed which when combined with the impact <br /> <br />veloci ty parameterization of Rasmussen and Heymsfield <br /> <br />(1985) <br /> <br />predicted the observed accretional density accurately. <br /> <br />2.2 REVIEW OF AOOREX;ATION THIDRY AND AOOREX;ATION MOOELS <br /> <br />2.2.1 Aggregation theory <br /> <br />Aggregation is a process of snowflake growth due to collision <br /> <br />and subsequent adhesion of ice crystals with ice crystals, ice <br /> <br />crystals with snowflakes, and snowflakes with other snowflakes. <br /> <br />Early radar observations have shown that aggregation is an <br /> <br />important precipitation process (Austin and Bemis, 1950; Wexler <br /> <br />and Atlas, 1956). <br /> <br />Ice crystal aggregation is a complicated <br /> <br />multifaceted hydrodynamic and electrostatic process canplicated by <br /> <br />the myriad shapes and sizes of crystals. <br /> <br />Laboratory observations <br /> <br />of models of ice crystal determined the conditions for two <br /> <br />crystals to aggregate (Podzimek, 1968). <br /> <br />. <br /> <br />8 <br /> <br />. <br /> <br />e <br /> <br />. <br /> <br />. <br /> <br />e. <br /> <br />. <br /> <br />e. <br /> <br />. <br /> <br />. <br /> <br />e <br /> <br />., <br /> <br />. <br />