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<br />-14-\8 -22 -26 -30 <br />500 Me TEMPERATURE l"C) <br /> <br />Figure 39. --Solid Lines: Mean Daily Snowfall at Wolf <br />Creek Pass as a function of cloud top temperatures <br />(500 mb). Dashed Lines: Adiabatic condensate <br />realized from lifting a parcel upward through a satu- <br />rated 700-500 mb layer. <br />~ u; <br />1-_ W <br />~~ 6 0,6 <br />UJ~ 2- <br />~:;; --' <br />U)S .J <br />150:: 4 ~,4 <br />~~, ~ <br />u--' '" <br />;::!~ 2 ~ ,2 <br />~8 g <br />~~.., <r <br />~~ 0 ~ 0 <br /> <br />~- u; <br />;?;~6 ~ ,6 <br /> '" ~ <br />~~ --' <br />",9 --' <br />Z0::4 ! 4 <br />~w <br />Z~ <br />8--' '" <br /><i~2 ~ .2 <br />~ <br />~~ ~ <br />w' <br />b80 W 0 <br />a..... =< <br /> 8 ,8 <br />W Cii <br />::I: W <br />1-- ::I: <br />z=< ~ <br />-~6 ,6 <br />w..... <br />~~ --' <br />,.J <br />"'- ~ <br />za: <br />wW4 ~ 4 <br />~~ Z <br />0--' (/) <br />u <br /> co ~ <br /><i~2 <i ,2 <br />~~ 0 <br />2 <br />~~O <{ <br />W <br />:;; 0 <br /> -10 <br /> <br />10 <br /> <br />W <br />~ <br />~ <br />2 <br />W <br />u <br />cr <br />W <br />a. 5 <br />W <br />> <br />t;i <br />--' <br />W <br />0:: <br /> <br />(a) <br /> <br /> <br />(b) <br /> <br /> <br />[POTENTIAL alNDENSATE <br />_ MEAN DAILY SNOWFALL <br />--- <br /> <br /> <br />( b) <br /> <br />r------, <br />1 I <br />I ... PERCHITAGE OF TOTAL <br />I I SNOWFAll <br />I 1 <br /> <br />FREQUENCY CF OCCURRENCE <br /> <br />,----- <br />1 <br /> <br /> <br />o -10 -14 -18 -22 -26 -38 <br />500 MB TEMPERATURE lOCI <br />Figure 40. --(a) Mean Daily Snowfall at Wolf Creek <br />Pass as a function of cloud top temperature (500 mb). <br />(b} Distributions of total snowfall and total occur- <br />rences as a function of cloud top temperature (500 mb). <br /> <br />rather steadily to the limit of the data around <br />_340 C. It is interesting that if this trend is <br />extrapolated the mean daily snowfall reaches <br />zero at about _370 C. This is thetemperai:ure where <br />observations by Smith and Heffernan (1954) <br />indicate concentrations of effective natural ice <br />nuclei are approximately equal to cloud droplet <br />concentrations. As a consequence, immediate <br />icing of the cloud would result in cessation of <br /> <br />I <br />i <br /> <br />the precipitation process. : <br /> <br />The decrease in mJan snowfall as <br />cloud top temperatures beconie colder than -230 C <br />is largely explained by the detrease of potential <br />condensate in the cloud syste~. This is illus- <br />trated in Figure 39 by the das;hed lines which <br />reflect the amount of adiabati~ condensate pro- <br />duced by a parcel moving upV;ard through a 700- <br />500 mb saturated layer as a function of the 500 <br />mb temperature. I <br /> <br />The peak in mean cj.aily snowfall at <br />-230 C appears to reflect a c~oud top temperature <br />mode where the condensation, supply and available <br />effective ice nuclei maximiz~ the precipitation <br />process. ! <br /> <br />-38 <br /> <br />The decrease of mean daily snowfall <br />as cloud top temperatures become warmer is <br />quite intriguing. The mean cj.aily snowfall <br />decreases steadily from _230, C to a minimum <br />about _180 C. This occurs irt spite of an increase <br />in potential condensate for these cloud systems. <br />This decrease cannot be explained qy a lessening <br />of any orographic influence siince an increase in <br />southwesterly flow events and increasing wind <br />speeds occur within this temperature range. It <br />appears the natural precipita'tion process is <br />becoming increasingly ineffi~ient as temperatures <br />decrease from _230 C to -18~ C probably due to <br />the accompanying exponentiail. decrease of <br />available effective ice nuclei'. <br /> <br />The marked incre~se of mean daily <br />snowfall at Wolf Creek Pass for 500 mb tempera- <br />tures around _140 C to _~50 C is striking. <br />However, since this occurs p.ear the tail of the <br />distribution, sample sizes are relatively small. <br />Possible explanations for th~s peak do exist. <br />One possibility is that this is the range of <br />temperature where dendritic crystal habits might <br />be expected to form in the upper portion of the <br />~ cloud system. This could result in fracturing <br />of the dendritic crystals and: an ice crystal <br />multiplication process in th~ cloud system. This <br />should cause an increase in ithe natural efficiency <br />of cloud water removal and therefore in observed <br />precipitation. Whatever the mechanism for this <br />increase in natural snowfall! efficiency at Wolf <br />Creek Pass, it apparently occurs less frequently <br />at Climax. Figure 37 indicates only a minor <br />peak in mean daily snowfall at Climax at these <br />temperatures. <br /> <br />It is interesting 1tnt the mean daily <br />snowfall appears to decrease again at the warmest <br />cloud top temperatures contained in the data <br />(_110 C to _130 C). However, with the limited <br />sample size::; involved this rs only conjecturc. <br /> <br />Figure 40 shows ];1ow the total snowfall <br />and the total occurrences are distribvted with <br />respect to the 500 mb temperature. It is seen <br />that 46% of the total snowfall and 37% of the <br />total occurrences are contained in the class <br />interval from -20.50 C to -24.50 C. The 9% <br />excess of tre relative snowfall percentage over <br />the relative frequency in this class reflects the <br /> <br />54 <br />