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Last modified
7/28/2009 2:37:28 PM
Creation date
4/16/2008 10:37:08 AM
Metadata
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Template:
Weather Modification
Contract/Permit #
14-06-D-6467
Project Name
Weather Modification Pilot Project
Title
Weather Modification - A Pilot Project - San Juan Mountains, Colorado River Basin - Final Report
Date
2/1/1974
Weather Modification - Doc Type
Report
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<br />, <br /> <br />I <br /> <br />i <br /> <br />In other cases, ice growth by vapor deposition proceeds at a rate <br />sufficient to use cloud water as it condenses. In some weathe~ <br />situations, the supply of ice crystals can be so great that particle <br />growth is restricted by water availability and fall trajectories <br />of the ice crystals relative to the ground may be adversely <br />affected. <br /> <br />These concepts have been specifically tested (Grant and Mielke, <br />1967;Grant et aI, 1968; Chappell, 1970; Jiusto and Holroyd, 1970 <br />and 1971) and are demonstrated in Figure 1. <br /> <br />i <br /> <br />i <br /> <br />~ <br /> <br />I. <br /> <br />I <br /> <br />0.7~ I <br />- ;.. Icraqc <br />- - - - .c./~raqe <br /> <br />Rate of Co"~cnsation , <br />Difrusional Gro~th Rate of Ice <br /> <br />I <br /> <br />0.6 <br /> <br />---0-- Average Preclpitatio~ Observea (no: see';ed cnses) <br />---...--- A,erage Precipltatisn Ooserv",j (seeded c~.5es) <br /> <br />- <br /> <br />VI 0.5- <br />UJ <br />'" <br />U <br />Z <br />- <br /> <br />Average Condensation Rate USln, 10.1 Prec.ipitation <br />Hours/Day "lith Upward Speed O' 11.8 cm./:.ec. at <br />-200 C Ad.lUsted at Other Ter'c,=ratures Ac:ordinQ <br />:-.; .Q(ldtl01l~ vi tnt: r:ori~:ontal __lnd SpF.ed <br /> <br />I <br /> <br />>- <br />"" ,.. <br />c 0.4 <br />z: <br />0 <br />~ <br />'" <br />t- <br />e: <br />u <br />UJ 0.3 <br />0:: <br />Q. <br />ex: <br />UJ <br />Q. <br />t- <br />~ <br />..J <br />c( 0.2 <br />:- <br />=> <br />0 <br />UJ <br />0:: <br />UJ <br />t- <br />"" <br />3 <br /> 0.1 <br /> <br /> <br />For 460 HB Cloud Top <br />..)Iith r:atural lee Nuclei <br />Spectrum <br /> <br />8 <br /> <br />II <br /> <br />( <br /> <br />II <br /> <br />b <br /> <br />c <br /> <br />II <br /> <br />.~.-. <br />..' <br /> <br />I <br /> <br />Number of Days <br />4 10 18 <br />4 7 15 18 <br /> <br />14 19 29 22 14 <br />16 27 28 17 <br />I <br /> <br />13 <br /> <br />o <br />-35 -30 <br /> <br />-25 -20 <br /> <br />-15 <br /> <br />-10 <br /> <br />II <br /> <br />FiSure 1. Di~tribution of non-sE!cded precipitation at H....~O as ~ <br />function of SO~ mb tcn;~~rature compared to a theor~tlcal distri- <br />bution cur;;putt:>d usinS" the mean diffu<.:;ional model. Precipitation <br />data are from Climax I sample (251) and values are a running mean <br />over a three-Jegree tetllperatllre interval. <br /> <br />- <br /> <br />Curve A in Figure 1 shows the rate at which water can be consumed <br />by mountain clouds with various cloud top (500 mb) temperatures <br />assuming: (1) clouds with characteristics of those observed near <br />Climax, Colorado; (2) ice crystal concentrations comparable to <br />concentrations of natural ice nuclei activated at the respective <br />temperatures, and; (3) a growth rate of individual crystals <br />determined by Chappell (1970) based on the ice diffusional growth <br />equations. Curve B, for comparison, shows the mean rate at which <br />condensate becomes available for clouds with various 500 mb <br /> <br />II <br /> <br />II <br /> <br />- <br /> <br />- <br /> <br />5 <br /> <br />~ <br /> <br />c..l <br />
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