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<br />10 <br /> <br />Jayaweera and Mason (1966) suggested that since snowflakes are <br /> <br />not often observed at <br /> <br />o <br />temper a tures colder than -5 C, <br /> <br />the <br /> <br />"cementing" of ice crystals by sintering* or by' capture of <br /> <br />supercooled drops may serve to keep warmer aggregates intact. <br /> <br />Aggregates which form in colder clouds contain less cloud <br /> <br />droplets; thus they are not cemented and may subsequently be <br /> <br />broken apart by coil isions or turbulence. <br /> <br />However, from <br /> <br />observations of Ohtake (1970), even large aggregates of dendritic <br /> <br />crystals did not exhibit any riming: <br /> <br />a direct contradiction with <br /> <br />Jayaweera and Mason (1966). <br /> <br />Ohtake suggested that the most <br /> <br />impor tant fac tor in crysta 1 agg regation is the mechan ical <br /> <br />interlocking between crystal branches. <br /> <br />Rogers (1974) documented that maximum snowflake diameters and <br /> <br /> <br />snowfall rates exhibited their greatest value near OOC. Snowflake <br /> <br />collection efficiencies were inferred to increase with surface <br /> <br />temperature to near uni ty at OOC. Ice crystal concentrations <br /> <br />necessary for aggregation to maximize snowflake diameters were <br /> <br />calculated to be in the range 103 to 105 m-3. <br /> <br />The number and <br /> <br />sizes of ice crystals which comprise aggregates were related to <br /> <br />the overall sizes of the aggregates. <br /> <br />Rogers suggested that large <br /> <br />dendri tes (5 rrm) exhibit unstable fall behavior, characterized by <br /> <br />horizontal excursions during descent; the sweep out volume, <br /> <br />consequently increased, estimated to be by a factor of 5. <br /> <br />* Sintering IS the diffusion transport of water molecules to <br />reg ions of large curvature; the transport is driven by the <br />gradient of the surface free energy. <br /> <br />. <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 />