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Last modified
7/28/2009 2:40:26 PM
Creation date
4/24/2008 2:49:21 PM
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Template:
Weather Modification
Title
The Practicability of Dry Ice for On-Top Seeding of Convective Clouds
Date
1/1/1978
Weather Modification - Doc Type
Report
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<br />. <br /> <br />I <br /> <br />JANUARY 1978 <br /> <br />H 0 L ROY D, SUP ERA N D S I LV E R.M A N <br /> <br />57 <br /> <br /> <br />. <br /> <br />poorly sampled. On two other days with CO2 seeding <br />some natural clouds, usually dissimilar to the seeded <br />clouds, were also sampled. Those days, however, are <br />also days excludable for poor sampling of the seeded <br />clouds or for suspected ice multiplication. Cloud 1 <br />on 8 December 1972 was a noteworthy layer cloud in <br />that the only snow observed to fall anywhere in the <br />region of this altocumulus cloud was from the seeded <br />line. In summary, it is possible that some of the ice <br />crystals sampled in the seeded cloud in the Australian <br />experiments resulted from causes other than seeding. <br />In Table S the air temperature at the seeding level <br />can be considered to approximate the cloud-top <br />'temperature at the time of seeding; the true value may <br />be up to SOC colder, as in the 8 July 1976 case. None of <br />the adequately sampled clouds appreciably increased <br />their cloud-top altitude after seeding; so for them the <br />seeding level temperatures also approximate the coldest <br />temperatures achieved. Cloud-top temperatures may <br />also be approximated by multiplying the cloud thickness <br />above OOC in Table 4 by a moist adiabatic lapse rate <br />appropriate to the region of SOO mb and - lOoe. The <br />Australian experiments lacked temperature soundings <br />above the flight levels, so that the true cloud top <br />temperatures are unknown for those cases. Cloud-base <br />temperatures for all experiments were at or warmer <br /> <br />, <br />I <br />e <br />I <br /> ... 0 <br /> \I) <br /> ct <br /> 1&I en <br /> CI) <br /> E .... <br /> oX <br /> ..10 <br /> UJ <br /> 0 <br /> Z <br /> ~ <br /> (f) <br /> 5 <br /> w <br /> > l\I <br /> j:: <br /> <t <br /> ..J <br /> W <br /> Q: <br /> 0 <br /> ... ;- <br /> \I) <br />f I&J <br />~N <br /> 2340 <br /> <br />KEV: <br /> <br />LIQUID WATER CONTENT <br />I .- <br />0..02 ()5 2 4gm-3 <br /> <br />than O"C except for 8 December 1972 cloud 1. Base <br />temperatures could not be monitored during the <br />single-aircraft Australian experiments. ' <br />The four reliable American experiments show an <br />average nucleation effectiveness of about 2 X 1011 <br />crystals per gram, using the Mee and Eadie (1963) <br />sublimation rate. Using the Fukuta et at. (1971) <br />sublimation rate raises this average to SXlOll. These <br />estimates are supported by the reliable Australian <br />values, which average a factor of 6 lower but which <br />must still be normalized upward to correct for the <br />expected lower crystal counting efficiency of the foil <br />impactor. Corrections for the absolute ice particle <br />sampling efficiencies for all instruments and for the <br />numbers of crystals within aggregates have not been <br />applied and should raise the effectiveness values further. <br /> <br />5. Discussion of the 8 July 1976 experiment <br /> <br />A pa.tch of tall altocumulus clouds was selected for <br />dry-ice seeding on 8 July 1976. There were no towering <br />cumulus clouds in the area capable of raining to the <br />ground. There were a few cumulonimbus clouds visible <br />over 100 km away to the north and northwest. <br />Four aircraft were involved in the study. The seeder <br />and a doud physics aircraft were near cloud top and <br /> <br />ICE PARTICLE CONCENTRATION <br /> <br />I I I <br />o 40 80 160 (I <br /> <br /> <br /> ..... <br /> r <br /> . . <br /> . '. <br /> 0, '" <br /> ..... '" '.,,' <br /> i ~i i <br /> 13 /5 /7 <br />55 0000 05 10 15 20 25 30 35 0040 <br /> TIME., GMT <br /> <br /> <br />FIG. 4. A length-time diagram of the seeded cloud of 8 July 1976. The Cloud was penetrated through the center of the cloud at the <br />indicated times in a generally east-west orientation. The heavy line represents the boundaries of the liquid cloud; the shaded regions <br />give contours of liquid water content. The thin line represents the boundaries of the ice cloud; the segmented lines and the interior thin <br />solid line give the contours of ice crystal concentration. Mid-level convection continued to stir the crystals and regenerate the liquid <br />cloud for nearly 1 h. . <br /> <br />l~.,l":ii "'~"" . ..:.'f,',': ,i..' ,.;, ,,;"'';;,i.i... ".' .... <br />,..., :, '"'~'"", '=,"".lL~V,">'A'%'.d ","..; ,:,.j,.(l;~.:, c. ......€i,;iiliIl"i:"""."..,;"""....,'......,. :....:. .,) <br />-..~ "","",.;.~_~,' ..~."" :"-"'1s-.~::-~~t.:::.;.." <br /> <br />
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