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<br />6 <br /> <br />TABLE I <br /> <br />HIPLEX-l primary response variables <br /> <br />1. C1C 2, Cloud ice concentration, 2 min after treatment <br />2. CIC 5, Cloud ice concentration, 5 min after treatment <br />3. CCR 5, Concentration of crystals rimed, 5 min after treatment <br />4. PIC 8, Precipitating ice number concentration, 8 min after treatment <br />5. MVD 8, Mean volume diameter of precipitating ice particles, 8 min after treatment <br />6. AWC 8, Average liquid water concentration, 8 min after treatment <br />7. TFPI, Time to first precipitating ice (particles with diameters> 0.6 mm in concentra- <br />tions > 0.1 I.') <br />8. TFE, Time to first radar echo (15 dBZ) <br />9. (a) TIPA, Time to initial precipitation at +10oC level, aircraft measurement <br />(b) TIPR, Time to initial precipitation at +lO'C level, SWR-75 radar (15 dBZ) <br />10. (a) RERA, Radar-estimated rainfall at +10oC level, Z-R relationship adjusted by <br />hydrometeor measurements <br />(b) RERC, Radar-estimated rainfall at +10oC level, using a constant Z-R relationship <br />(c) AER, Aircraft-estimated rainfall at + 1 00 C level <br /> <br />CURRENT VIEWS ON POTENTIAL FOR RAINFALL AUGMENTATION <br /> <br />Canvective pracesses, including rainfall, are daminated by synaptic and <br />mesa scale systems which cantral claud size and arganizatian. Observatians <br />to. suppart this statement have been reparted fram Flarida (Ulanski and <br />Garstang, 1978), Texas (Tex. Dep. Water Resaur., 1982) and Mantana <br />(Miller et al., 1981). In general, canvergence values af 5 X 10-4 S-l ar mare <br />(in absalute terms) aver several hundred square kilameters are required to. <br />produce a majar canvective starm. The mesa scale canvergence is assaciated <br />with air rising at rates appraaching 0.5 m S-l in the lawer trapasphere. <br />Matthews and Silverman (1980) have used a numerical madel simulatian to. <br />demanstrate haw mesascale lifting increases the ability af the atmasphere <br />to suppart deep, maist canvectian. <br />Mast canvective rainfall is praduced by clusters ar lines af canvective cells <br />which require mesoscale suppart, rather than by isalated cells. Table II, <br />based an Jurica et al. (1981), illustrates the paint far west Texas. The small <br />amaunts af rainfall cantributed by is alated canvective clauds is attributable <br />to. the relatively small amounts af water vapor candensed in such clauds and <br />their law precipitatian efficiencies. <br />It has been suspected far a lang time that is alated cumulus clouds are in- <br />efficient precipitation praducers because they are dissipated by mixing with <br />ambient dry air befare the claud draplets have sufficient time to. caalesce <br />into. raindrops ar be collected by salid hydrometears (Braham, 1981). Evi- <br />dence an this point campiled by Canadian researchers (Schemenauer et aI., <br />198!.) during experiments in Ontario. and the Narthwest Territories and <br />during the HIPLEX experiments at Miles City is shawn in Table III. The set <br />of 'Miles City' clauds referred to in Table III is nat the same as the set af <br />