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<br />I <br /> <br />32 <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />'[ ,,'"U <br /> <br />5 <br /> <br />----------- - -------- _._--~ <br />----. .--- -----~--::- ~ <br />tCE CHYSTAL.--o--_ ,,~,- ~'-..., <br />Tf<AJECTORJES ---__ ~~ ............ <br />~_~~----- ,LWC.<:O.l <br /> <br />\_----_._--=--~-._,,~ ~.-::>(~-- ~ ~ <br />-'---~-:::..- -~;-~'~ <br /> <br />. .~, . ..~. 0 0 ~/~~~~/ <br />BLOCKED FLOW _/ / 1// /; / <br />2 ~77T/ / / / / l777 / / / t-1ARGET AREA-i <br />7/ ,10 KM <br />/ , f---------i <br /> <br />4 <br /> <br />a <br /> <br />G <br /> <br />NEUTRAL BeLOW CLOUO <br /> <br />4 <br /> <br /> <br />b <br /> <br />~ ~ <br />~ -=- <br />4;;1J7177777m~ <br /> <br />G <br /> <br />UNSTABLE <br /> <br />:l; <br />'" <br /> <br />~-- <br />/ 0 ~.------==~~ ~ <br />--- ~~~ <br />>_ - L we -..c..... <br />__ __ __ ___ .~ /,~-----'-Q5_J.o '~ <br />~~---- / "" ---'-. <br />-....., >- ""') "- <br />_~ }WC;::'22.-:9,.5_ .:;.,....--...-r " <br />------- "'--" ,/, .-~ <br />-'7- 0--""'....." <br /> <br />~..:~/~"u~,<Y~ /.....y'- ;;- ~j_________ <br />~,--O,ls,~~~ "(,. / ~ <br />/" u <br />.-----------=============--- <br /> <br />~~/ 10 KM <br />1-------< <br /> <br />c <br /> <br /> <br />-~- <br /> <br /> <br />k:-TARGn AREA-->I <br /> <br />Figure 3.5. This figure is the same as Fig. 3.3, \.;rith the addition of <br />some possible ice crystal trajectories (dashed lines \.;r1.th <br />arrmvs). The farthc~~t dO\Vflwincl (farthest. right) trajectory <br />shows the fnll of a crystal with a terminal velocity of <br />1. m/ ~;t~C. All other traj ectorics originate as 10 111ll Pla <br />crYf,tal~; and Grow and fall accord ing to the equations of <br />Davis (1974). <br />