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<br />-. <br /> <br />,! <br />~ <br />\"'. <br /> <br />/' <br />( <br /> <br />\ <br /> <br />C.' <br /> <br />';;' .,.', ," ., <br /> <br />". <br /> <br />. . . .'~ .: ~;" ;i.:_'.~.~~~~~l'Qi,~~t~~:t ~/ ~'t:j;'~4:' <br /> <br />. . \.. <br /> <br /><I <br /> <br />Cloud liquid Water Content. February 9.1984 <br /> <br />30 <br /> <br />r ..... >0.1 Lwe <br /> <br />i <br />- <br /> <br />i <br />!20 <br />I <br />iii <br />e <br />cr <br /> <br /> <br /> <br />.00 ,05 .10 .15 .20 .25 .30 .35 .40 .45 .50 <br />Cloud liquid water content (g/m3) <br /> <br />Figure 2. Frequency distribution of "in-cloud" <br />liquid water content for cloud penetrations made <br />on February 9. 1984. <br /> <br />~.3 Cloud Precipitation Conversion Efficiency <br /> <br />Estimates of the precipitation conversion <br />efficiency of the winter clouds for selected days <br />were made as indicators of the general seeding <br />potential. Conversion efficiency was defined as <br />that portion of the upwind llOisture converted to <br />precipitation-sized particles in the clouds over <br />the mountain region. This percentage was <br />expressed as the ratio of the average ice water <br />(r.lelted ice mass) of precipitation-sized <br />particles within the clouds to the available <br />vapour supply. This approach is sirni1ar to that <br />of a previous case-Study analysis of an <br />orographic cloud systeD measured in 1982 <br />(Krauss et al., 1983). It is interpreted as a <br />relative-esfimate, and not of the overall <br />efficiency of the removal of condensed water from <br />the clouds (e.g. Dirks, 1973). <br /> <br />Three days were selected for this <br />analysis, one fro~ each of the three field <br />seasons: March 15th and December 9th, 1983 and <br />February 9th. 19R4. These three days were <br />characterised by clouds lIfith bases at or below <br />the mountain ridge line, extending from the <br />western edge of the Rocky Mountain massif and <br />across the continental divide. The clouds of the <br />F ehruary and December cases were genera lly <br />shallow stratifom while the March case include <br />SOllIe cumulus type clouds. Winds at cloud level <br />were predominantly westerly. Surface <br />meteorological stations located along the flight <br />tracks reported light snow during the aircraft <br />measurement periOdS. <br /> <br />'. <br /> <br />Aircraft "in-cloud- .easurements were <br />along the east-west flight track (Fi gure 1, <br />leg C), venera lly at the 11,000 to 12,000 feet. <br />level and with temperatures ranging from _130C <br />to about -20oC. Cloud precipitation-sized <br />particles were Measured using a PHS 2D-P probe. <br />A precipitation-sized particle was defined in <br />this study as any particle greater than 20U <br />microns in diall\eter, the minimum detectable size <br />of this instrument. All 20-P data was processed <br />for a one-second averaging period, and the <br />complete data set for one east-to-west pass was <br />then averaged to derive a mean precipitation <br />particle diameter and concentration for the <br />"in-cloud" data. <br /> <br />The 2D-P measured mean particle paraneters <br />can be use~ to estimate the mean ice water <br />content of the cloud regi(\n. Particles were <br />assumed to be thick plate crystals. The mass of <br />the individual particles was estimated using the <br />empirical diaMeter 0 (c~) to volume V (c~3) <br /> <br />relation suggested by Pruppacher and Klett (1978, <br />p. 40): <br /> <br />V .. 0.0897 D2.778 <br /> <br />Assuming an average density of 0.9 g/c~3 for <br />hexagonal plates (ibid, p. 41), the diameter to <br />mass M (g per particle) relation is: <br /> <br />H .. 0.OB07 02.778 <br /> <br />The average total unit volume ice water mass "t <br />(g/m3) of the cloud sample leg is then expressed <br />as: <br /> <br />Ht .. M · Np <br /> <br />where Np (particles per <br />precipitation particle <br />sample. <br /> <br />m3) is the <br />con cent rat i on <br /> <br />average <br />of the <br /> <br />Total ~isture available to the cloud was <br />est imated using the Ilost representative upwind <br />radiosonde sounding coincident with aircraft <br />measurements. For three case studies, the <br />selected sounding was made from the Cranbrook <br />British ColUlllbia upper air site within two to <br />three hours prior to the aircraft measurenents. <br />This valley site is approximately 100 kilometres <br />west of the continental divide and is the western <br />endpoint of the flight leg. The calculated <br />upwind atmospheric water vapour content for the <br />cloud layer of ~ach of the three cases was 1.0, <br />2.2 and 2.0 gIn' respectively. These values do <br />not account for entrainnent effects and are <br />viewed as upper limits of the parcel water vapour <br />available to the cloud. <br /> <br />Calculations for the three days yielded <br />the following estimates of cloud precipitation <br />conversion efficiency: <br /> <br />March 15, 1983 - ~ to 13~ <br />December 9. 1983 - 16~ <br />February 9, 1984 - <IS to 1J <br /> <br />The ranges for the March and February cases <br />reflect the two data sets used for each date and <br />the Decet'lber value represents the single <br />continuous "in-cloud" data set used. <br />