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<br />1884 <br /> <br />100 <br /> <br />JOURNAL OF CLIMATE AND APPLIED METEOROLOGY <br /> <br />VOLUME 22 <br /> <br />C> <br />z <br />ii: <br />lr <br />::> <br />/ <> <br />o <br />o <br /> <br />O>T~-IO.C <br /> <br />z <br />o <br />c; <br />W <br />lr <br /> <br />I- <br /> <br />~ 10-1 <br /> <br />I- <br />Z <br />o <br />o <br /> <br /> <br />CEllULAR, <br /> <br />lr <br />W <br />I- <br /><[ <br />~ <br />!:! <br />::> <br />a <br />::i <br />LL 10-2 <br />0 <br />>- <br /><> <br />z <br />w <br />::> <br />a <br />w <br />lr <br />LL <br /> <br />r--l <br />I <br />r--I <br />I <br />I <br />I <br /> <br />I <br />BANDEDI <br />I <br />L____ <br /> <br />AREA-WIDE <br />1'-'-'-'''1 <br />r'-'-'-'..i ! <br />, I <br />j_'_'_,J i <br />I i <br />i i <br />i i <br />,_,_,_, i <br />i <br />i <br />i <br />! <br />! <br /> <br />['-'-'-' <br />I <br />i <br />i <br />i <br />i <br />i <br />i <br />i <br />i <br /> <br />w <br />> <br />f= <br /><[ <br />...J <br />W <br />lr 10-3 <br />1 2 4 B 16,32 64 12B <br /> <br />a WIDTH OF liQUID WATER CONTENT REGION (km) <br /> <br /> 100 <br />C> <br />z <br />ii: <br />lr <br />::> <br />0 <br />0 <br />0 <br />Z <br />0 <br />c; <br />W <br />lr <br />I- <br />Z 10-1 <br />W <br />I- <br />Z <br />0 <br />0 <br />lr <br />W <br />I- <br /><[ <br />~ <br />!:! <br />::> <br />a <br />...J <br />LL 10-2 <br />0 <br />>- <br />0 <br />z <br />w <br />:::> <br />a <br />w <br />lr <br />LL <br /> <br />T<-10.C <br /> <br /> <br />CELLULAR <br /> <br />1 <br />I <br />J <br /> <br />I <br />I <br />I <br />I <br />IBANDED <br />I <br />I <br />I <br />I' <br />I <br /> <br />w <br />> <br />f= <br /><[ <br />-' <br />W <br />lr 10-3 <br />1 2 4 8 16 32 64 128 <br />b WIDTH OF LIQUID WATER CONTENT REGION (km) <br /> <br />AREA-WIDE <br />i i <br />i i <br />i i <br /> <br />FIG. 11. (a) Distribution of the extent of regions of cloud where LWC > 0.2 g m-3 at temperatures from 0 to - lOoC shown for the <br />area-wide, banded and cellular echo combinations; (b) same as in (a) except temperatures less than - lOoC shown, <br /> <br />" <br /> <br />e. Stratification by 700 mb trough passage <br /> <br />This section examines the relationship between the <br />relative frequency of LWC/ICC ratios> 10 ""g per <br />crystal and the 700 mb trough environment. Both <br />Hobbs (l975a,b) and Lamb et al. (1976) have alluded <br />to a relationship between the occurrence of high LWC <br />and the postfrontal air mass. The results of this analysis <br />not only reveal this relationship, but also a certain <br />tim~ dependency. The 700 mb trough position was <br />obtained from time section analyses of rawinsonde <br />data. <br />Figure 12 shows the relative frequency that L WC <br />exceeded 10 ""g per crystal by observation temperature <br />in the post-trough environment. Maximum relative <br />frequencies of birge L WC/ICC ratios usually did not <br />exceed 0.2 in the pretrough observations. The relative <br />frequency that LWC/ICC ratios exceeding lO""g per <br />crystal were observed did not exceed 0.2 until 7 h after <br />700 mb trough passage. Recall that the occurrence of <br />the C 1 PET peaked at this same time. The relative <br />frequency maximum is sloped from a temperature of <br />approximately -150C at 7 hafter passage, to OOC, <br />9 h after trough passage. This may indicate deterio- <br />rating, convective conditions with time, resulting in <br />shallower clouds with warmer tops. Beyond 10 h after <br /> <br />trough passage relative frequencies dropped below 0.2. <br />The optimum time that large relative frequencies were <br />encountered ranged from 7 to 10 h after 700 mb trough <br />passage. <br /> <br />6. Conclusions <br /> <br />The results have provided a close look at the su- <br />percooled L WC and ICC in winter storms of the central <br />Sierra Nevada for the two successive years, 1978-80. <br />It should be mentioned that minimum observed clear- <br />ance altitude restrictions prevented the aircraft from <br />flying within - 1 km of the Sierra terrain,' and it is <br />possible that large LWC exist in this layer. <br />The cellular echo types clearly exhibit the most de- <br />sirable characteristics of significant liquid water and <br />relatively little ice. The extent of this region is bounded <br />in the vertical by the 0 to -150C isotherms and its <br />core 40 to 100 km upwind ofthe crest. The horizontal <br />extent of significant L WC was also greatest within the <br />cellular PET, with segments 32 to 64 km wide fre- <br />quently measured. <br />The area-wide and banded echo types provide fewer <br />instances of significant supercooled water and absence <br />of ice. L WC were strictly confined to the higher tem- <br />