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Last modified
7/28/2009 2:40:11 PM
Creation date
4/23/2008 1:57:54 PM
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Weather Modification
Title
The Use of Microwave Radiometry to Determine a Cloud Seeding Opportunity
Date
9/9/1982
Weather Modification - Doc Type
Report
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<br />SEPTEMBER 1982 <br /> <br />J. B. SNIDER AND D. ROTTNER <br /> <br />1289 <br /> <br /> <br />Yuba City <br /> <br />t <br /> <br />VIRGINIA <br />""^ <br />RANGE tv" <br />1\ <br />tIY./ <br />""" <br />Washoe -it'.,0 <br />Lake ~ tfjJ- <br />PY! <br /> <br />~ 0 10 U 20 <br />~ ee 'SCALE Of MILd = <br />E r"''v~ <br />~ J/?' 5 0 5 10 U 20 <br />~ SCALE' 0; KILOMETiRli <br /> <br />FIG. 2. Map of SCPP teslt area showing propagation path to COMST AR satellite. Numbered triangles mark locations of <br />three regions seeded on 3 March 1980. <br /> <br />6. 3 March 1980 seeding experiments <br /> <br />On the morning of 3 March 1980, an overcast com- <br />posed of non-precipitating stratiform clouds covered <br />the test area including the region of sky observed by <br />the radiometer. At 0745 PST (1545 GMT) the radio- <br />metric system indicated ~- 1 mm of total liquid (Fig. <br />1). However, both 5 cm radars observed few if any <br />echoes. Since liquid water was detected by the radi- <br />ometer, the site director decided to launch the cloud <br />physics aircraft (N2UW) for measurements of L we <br />in the vicinity of the earth-satellite propagation path. <br />Table 1 summarizes the radiometric a~d in situ <br />aircraft measurements of doud liquid observed during <br />two flights near the propagation path. The first flight <br />was a descent from 3100 to 900 m; the second flight <br />.was an ascent over the same height interval. Both <br />flights were along a 1350 radial extending from the <br />Sheridan site. <br />For the comparison shown in Table 1, the mea- <br />sured data have been converted to the average L we <br /> <br /> <br />(g m-3) contained in an equivalent vertical column <br />through the clouds. The path-integrated liquid data <br />(mm) recorded by the radiometer were converted to <br />averagl~ L we using a cloud-thickness estimated from <br />the aircraft data and from soundip.gs made at Sheridan <br />at 1500 and 1800 GMT. Liquid data recorded along <br />the flight path were averaged as a function of vertical <br />height. Very little ice was detected by imaging probes <br />carried on the aircraft. <br />Although similar L we's are obtained with the air- <br />borne and ground-based techniques, the radiometric <br />method shows somewhat higher values than were ob- <br />served by the aircraft probes. Surface observatIons <br />made near the flight times show the cloud ceiling to <br />be -600 m. Therefore, the radiometer may be de- <br />tecting liquid that is present below the minimum al- <br />lowable flight altitude of 900 m. Part of the difference <br />could also be caused by different paths being sampled <br />by the two techniques; the aircraft instruments sam- <br />pled cloud liquid along an _70 slope rather than along <br />the 32.60 elevation angle of the propagation path. <br />
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