Laserfiche WebLink
<br />1292 <br /> <br />POST-FRONTAL <br />LIQUID WATER <br /> <br />PRE-FRONTAL <br />LIQUID WATER <br /> <br />(WEST TO SOUTHWESTERLY <br />FLOW ALOFT) <br /> <br />(NORTHWEST TO NORTHERLY <br />FLOW ALOFT) <br /> <br /> <br /> <br />t&:& <br />&&& <br />t&&& <br />&&& <br />~ &&& <br />I ........ <br />&&& <br />t&&& <br />&&& <br />& & <br /> <br />& <br />& & <br />~~::& <br />& <br />& <br />& & <br />& <br />~........: <br />~&& <br />& & <br />& <br />~&&& <br />& & <br /> <br />FIG. 2. Schematic depiction of low-level windflow with respect to <br />the cold front for (a) storms traveling in a southwesterly flow aloft <br />with liquid water occurring post-frontally and (b) storms traveling in <br />a northwest to northerly flow aloft with liquid water occurring pre- <br />frontally. <br /> <br />SPLIT-FRONT MODEL <br /> <br />Km. <br /> <br />6 <br /> <br /> <br />3 <br /> <br />o <br /> <br />FIG. 3. Conceptual model of a split front and indicated regions of <br />seeding opportunity. (After Browning and Monk 1982). <br /> <br />in SLW (determined from radiometric measurements) associ- <br />ated with a corresponding drop in cloud top, a decrease in radar <br />reflectivity, and a decrease in precipitation rate at this same <br />location. <br />Competing processes can occur within shallow orographic <br />cloud systems. Release of latent instability by forced ascent <br />can develop pockets of natural ice. Strong evaporative cooling <br />near cloud top induced by mixing can lead to natural areas of <br />high concentrations of ice crystals. In addition, regions of co- <br />alescence-grown drops can lead to rapid glaciation by the Hal- <br />let-Mossop (1974) process. These processes together lead to <br />the high variability of SLW and ice observed in these cloud <br />types. <br />For storms moving in from a more northerly direction (me- <br />ridional flow), SLW generally occurs prefrontally. Here the <br />winds are more perpendicular to the barrier, causing an in- <br />creased low-level condensate supply and increased SLW. Post- <br />frontally, the winds veer to a northerly direction or "parallel" <br />to the mountain (see figure 2b). <br />When SLW exists it is necessary to know its amounts, du- <br />ration, and its vertical and horizontal extent. Aircraft obser- <br /> <br />, <br />""""~- <br /> <br />Vol. 69, No.1 1. November 1988 <br /> <br />26- 27 MAR 1985 <br /> <br />330 <br />II~____~---- ------ .---------.--TiJ~ <br /> <br />10 ---------~ /----~- ---,--------~---- 320 <br /> <br /> <br />(A) <br /> <br />.. <br />~ <br />~d <br />;:::E 5 <br />f~ <br />"~ <br />.~ .~ <br />~'" <br />"," <br /> <br />~--~_ . ._/290 <br />01 I --'-~I I <br /> <br /> <br />lill!:" i ;1,1 ,." ", .n >0' '" r I"' <br />0.0 -,-ii, ~,lJW~L,<\_'__,-uJ~~ <br />E 6.0.. ~'~ <br />i ~ ~ 4 0 _ 0 ~~.~9 _n_ "- <br />~~ ~ . _ :~~:~: _ j)~_ - _~ ~ -. ~ ~_o_Q ~ra~ <br />~~020-,-, , ,"3~2~, , , <br /> <br /> <br />HI : ~lrlIGI1'-~:~~I~)llllllllill_ljlfJ"'m'T~ I~_'_I_ (D) <br /> <br />15 12 09 06 03 00 21 18 15 12 09 <br />T I ME (UTe) <br /> <br />(e) <br /> <br />FIG. 4. Composite temporal analysis for the 26-27 March storm <br />crossing the central Sierra Nevada (time increases to the left), from <br />top to bottom; (A) 8, time-height from the Sheridan rawinsonde. Fea- <br />tures noted, WF (warm front), CF (cold front), J (jet maxima), and <br />scalloped line indicates cloud boundaries as estimated using relative <br />humidity, satellite cloud top temperatures, and the "Sheridan-radar" <br />cloud tops. Computed 2500 condensate supply rate integrated from <br />surface to 5 km over Sheridan is shown at the time of the soundings. <br />(B) Vertically integrated liquid water from the dual-channel microwave <br />radiometer at Kingvale. (C) Time-height radar-reflectivity profile over <br />Kingvale as determined by the Sheridan radar. Minimum detectable <br />signal over Kingvale is 8 dBZ. (D) Precipitation rate (mm . h-I) <br />measured by a weighing-type precipitation gauge at Kingvale (Reynolds <br />and Kuciauskas ] 988). <br /> <br />'lations have been used extensively to determine the spatial <br />variability of SLW, but only to within 500 to 1000 m of the <br />underlying terrain. The application of the radiometer within <br />various mountain locations allows determination of the tem- <br />poral variability of SLW and the direct comparison among <br />different geographical locations of integrated SLW observed <br />from cloud base through cloud top. Figure 5 shows the cu- <br />mulative distribution of SLW observed at three separate geo- <br />graphic locations.' Note that approximately 85 percent of the <br />time SLW is observed, it has a value below 0.2 mm. Using a <br /> <br />2 For this graph, data availability varied depending on the project. <br />For SCPP, 775 hours of SLW observations were available from four <br />seasons, ]983-84 through ]986-87. for CRADP, 958 hours of ob- <br />servations were available for the period November through December <br />]983 and January through March ]985. For Utah, 7]9 hours of ob- <br />servations were used for the period February through March] 985. This <br />distribution is similar to one produced using ] 79 hours of radiometer <br />data from the ]983 Utah field project. <br />