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7/28/2009 2:40:45 PM
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4/24/2008 2:55:08 PM
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Weather Modification
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Scientific Weather Modification Experimentation in the United States
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<br />project area that consists of a pr9ject <br />office and a ground based observing facility <br />known as the Grand Mesa Observatory. The <br />observatory has the capability to measure <br />state parameters at the surface and a height <br />of ~bout 20 meters. Other equipmenc at the <br />observatory includes a 5-cm radar, a dual <br />wave 1 ength mi crowave radi ometer tv measll re <br />liquid water, precip1tation gages, and <br />Particle Measuring System's 2-dimensional <br />cloud particle probe; Measurements above the <br />surface of the Mesa are made using an instru- <br />mented cloud physics aircraft. Initial <br />investigations (Holroyd and Super, 1984) have <br />confirmed the presence of supercooled liquid <br />water in sufficient ~uantities to indicate <br />that cloud seeding could potentially be suc- <br />cessful. Terrain. rather than ice particle <br />presence. appears to be the dominant <br />influence in determining the distribution of <br />liquid water over the slopes and top of Grand <br />Mesa (see Figure 7). The water appears to be <br />concentrated in the lowest levels and is pre- <br />sent in sufficient significent amounts only <br />for limited periods of time (mean = 3 h. <br />upper standard deviation =6.5 h). The pre- <br />sence of the highest liquid water in the <br />lowest levels may make ground seeding most <br />practical. <br /> <br />6. Related Research <br /> <br />a. Microwave radiometer <br /> <br />In the description of the CRADP and SCPP <br />programs. an instrument was described which <br />appears to have a high potential for <br />detecting clouds which are seedab1e. The <br />instrument is called a dual wavelength <br />radiometer and remotely senses the amount of <br />water vapor and supercooled liquid water that <br />is present in nearby, clouds. It does this by <br />passively measuring incoming microwave <br />radiation at wavelengths appropriate to water <br />vapor (20.6 GHz) and to liquid water (31.6 <br />6Hz). The brightness of the radiation is a <br />measure of the integrated water in that phase <br />along the line of sight. The computer- <br />controlled antenna which receives the signal <br />can be operated in a stationary or a scanning <br />mode. and the data are recorded on disk <br />and/or on tape. <br /> <br />A cross-section of the physical layout of the <br />system is shown in Figure 3. The electronics <br />for both the 20.6 and 31.6 GHz radiometers <br />are located in a single package. The mini- <br />computer is also located inside the trailer. <br />Equal beamwidths (2.50) are produced at both <br />fr~quencies. Mobility of the instrument is <br />~chieved by using an enclosed trailer as both <br />,-a small laboratory and an antenna platform. <br />A more detailed description of the radiometer <br />unit is found in Hogg et ale '(1983). <br /> <br />Several analyses have been performed to <br />determine the veracity of the radiometer <br />data. Westwater (1978) found the accuracy of <br />vapor values to be better than 15 percent for <br />a wide range of cloudy conditions. Guiraud <br />et a1.(1979) showed that the accuracy in <br />measurement of precipitable water vapor is <br />about the same or somewhat better than that <br />of operational radiosondes. He also found <br />that a considerable ,amount of vapor often <br />passes overhead unobserved by sondes. The <br />liquid measurements have been compared <br /> <br />. <br />_ __.q(Q.1St~, ijO <br /> <br />70 <br /> <br /> <br />:, <br /> <br />J() <br /> <br />c:.. <br /> <br />Ji <br /> <br />60 :, <br /> <br />30 <br /> <br />> <br />.... <br />'"' <br /> <br />E <br />::l <br />u <br /> <br />o km <br /> <br />-~; <br />T""~ I ,---~ <br />30 70 <br /> <br />100 <br /> :r. <br /> ~ <br /> rr. <br /> :L <br /> <'l <br /> C. <br /> '~ <br /> :: <br />50 ..., <br /> c <br /> (lJ <br /> i:: <br /> OJ <br /> c. <br /> <br />Key <br />both Figs. <br /> <br />rua..__ <br />0,2.4 gm-3 <br /> <br /> <br />3.7 km P"SSE'S <br /> <br />o ;.. <br /> <br /> <br />:G: <br /> <br /> <br />-50 <br /> <br />J~ <br /> <br />- 30 0 km <br /> <br />te r.r"in <br /> <br />30 SO <br /> <br />FIGURE 7 -- DISTRIBUTION OF LIQUID WATER OVER <br />GRAND MESA; TOP: ALONG AXIS. BOTTOM: <br />CROSS-AXIS (AFTER HOLYROYD AND SUPER. 1984) <br /> <br />Double Mylar, Cowling t <br />Window '\ -- : ~~ Elevation <br />" ./ ,....1....--, I ,... <br />AZlO'uth "15-:'" 7:' I 11'" - Flat <br />Flal . /', 11-,r-r.- 4:1 and <br />and -:' : ~ ~~:,.Ii' ;:-"-~:-- - Bearing <br />6ea~lng,,~ _~ ( ! __ ,]*~~ _., :; <br />-- - ----10~:-c--.-~~--:- - ~~~;o3~e~e~8HZ <br /> <br /> <br />t ~ ,--- -~- <br />r----j ; j II - -1 <br />bo~:;~,., t~' I?J_'j~ <br />L~:JJL __" }l::tt~~ld _8 <br /> <br /> <br />---:.;::-~-'- - -- ------- -- f <br />/ -,-~,--'\ <br />~~~J~) <br /> <br />, Side <br /> <br />I <br />L <br /> <br />FIGURE 8 -- SIDE VIEW OF ~ STEERABLE <br />DUAL-CHANNEL RAD IO'IETER SHOWl NG ~IECHANICAL <br />LAYOUT; A CENTRAL RAY FROM ZENITH IS SHOWN AS <br />DASHED LINES WITH ARROWS (AFTER HOGG ET AL. <br />1983) <br /> <br />..J. <br /> <br />, <br />... l,'. .,-~, ~ <br /> <br />a :3 . 't <br />f~~n?"t~w <br />~'."'fi~J, <br />
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