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<br />-:-.5-.. <br />..~ <br /> <br />j.- <br /> <br />.....-:~ : <br /> <br />l~ <br /> <br />Tho ~Q~n prer": -~ ~::::.t''': (";- r-"e tT;'l" C.l.....0 '!~) I-or "he> ~erl-d l~l U. ~O() T,.,rn <br />_u,- ".~c:..' ,--'-p~:",-_-,--.l." _CL. \1 O~L ~ .L.... '- ~ p . v. :;J~-ll u L~l is <br /> <br />D2se2 on r~O precipitatio~ gages in the SCPP. <br /> <br />The upwirrd edge tor the <br /> <br />r2i~fall ~as ~2a ~~ !ro~ ~~e CP-3 radar. <br /> <br />The meaD precipitation rate was <br /> <br />~ 1~ <br />~ea~~y unifor~ froc 25 to 75 km ra~ge. <br /> <br />In the zo~e from 25 to 75 km. the <br /> <br />iastc~:aneo~s rai~fall ra~es from t~e convect~ve storms are much higher <br /> <br />than the cea~ ~recip~tatio~ rate. <br /> <br />The sterns formed along the convective <br /> <br />line ~ear '20 k~, .a~~ moved ~p the barrier as they precipitated. The <br /> <br />i~~egrated effect was to produce a uniform mean precipitation rate over the <br /> <br />I <br />I <br />! <br />, <br /> <br />~idd:e part of the barrier. <br /> <br />Since the net effect from both this convective case and the previous <br /> <br />stable case was a unifo~m precipitation rate over much of the Sierra <br /> <br />barrier, it should not be surprising that the total annual precipitation <br /> <br />;~ <br /> <br />.' <br />,-- <br />I' <br />!::-- <br /> <br />over the upper half of the Sierra barrier is approximately uniform. <br /> <br />Flights through this and several other deep, unstable orographic storms <br /> <br />~ - - <br /> <br />1 <br />t <br /> <br />G~ring the early years of sepp indicated that the upwind edges of these <br /> <br />. <br />!- <br /> <br />cC:1vective <br /> <br />,. <br />_l.nes <br /> <br />were ice free and contained continental <br /> <br />dr,Qplet <br /> <br />ii_- <br />.- <br /> <br />! <br /> <br />~o~centratlons of <br /> <br />-3 <br />200 to 4QO cm <br /> <br />As the convective clouds ascended <br /> <br />through the -15 to -20oC level, natural ice developed. In the presence or <br /> <br />liquid wa:er conte~ts approaching adiabatic values, the ice ?articles grew <br /> <br />, <br />'0 <br />. <br />L: <br /> <br />rapicly by r~ming res~lting in lightning, graupel and small hail. Downwind <br /> <br />or the deeD cOGvection and over the upper half of the barrier, the cloud <br /> <br />; -- <br /> <br />L <br />. <br />i- <br />F <br /> <br />was totally glaciated. <br /> <br />j, <br />io ~ - <br /> <br />.' <br /> <br />34 <br />