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<br />----------.-- <br />TABLE II. --Estimate oJ scale changes during seeded periods with respect to <br />non-seeded periods as computed by three statistical methods. Scale changes <br />are shown as a function of the 700 mb mixing ratio. <br /> With Controls Without Controls <br /> Total Sample Scale Scale <br />Stratification Sample Size Change Change <br />(GM/KGM) Size Utilized Method (%) P- Value (0/0 ) P- Value <br />Climax I <br />O. 4 to < 1. 3 S 27 S 27 NP1 -28 . 171 < -50 .0392 <br /> NS 25 NS 25 NP2 < -50 .041 < -50 .0125 <br /> (S17,NS19) PAR -34 .115 <br />1. 3 to < 2. 8 S 72 S 72 NPl +7 .305 +13 .261 <br /> NS 89 NS 89 NP2 +10 .258 +19 . 147 <br /> (S56, NS70) PAR +14 .166 <br />2.8 to < 4. 6 S 21 S 21 NP1 +65 .071 +90 .138 <br /> NS 17 NS 17 NP2 +132 .255 +92 .206 <br /> (S17,NS13) PAR +35 .201 <br />Climax II <br />O. 4 to < 1. 3 S 14 S 14 NP1 -32 .291 -22 .264 <br /> NS 11 ' NS 11 NP2 <-50 .074 <-50 .108 <br /> (S8, NS8) PAR -52 . 171 <br />1. 3 to < 2. 8 S 36 S 36 NPl +23 . 187 +14 .298 <br /> NS 46 NS 46 NP2 -6 .409 +23 . 138 <br /> (S31, NS39) PAR +16 .224 <br />2.8 to < 4.6 Sl1 Sl1 NP1 +25 . 181 +180 .152 <br /> NS 9 NS 9 NP2 +164 .106 +118 .305 <br /> (S10,NS6) PAR +13 .421 <br /> <br />Wolf Creek Summit <br />O. 5 to < 1. 9 S 69 S 64 NPl -2 .480 -10 .409 <br /> NS 82 NS 79 NP2 -13 .323 -12 .334 <br /> (S34, NS45) PAR -9 .337 <br />1. 9 to < 2. 8 S 59 S 50 NP1 +45 .050 +48 .111 <br /> NS 76 NS 74 NP2 +66 .0197 +41 .113 <br /> (S33, NS51) PAR +58 .0040 <br />2.8 to < 5.2 S 36 S 33 NPl +57 .117 +165 .0183 <br /> NS 40 NS 28 NP2 +64 .127 +111 .053 <br /> (827. N825) PAR +54 .054 <br /> <br />Again the consistency of the three <br />independent samples is apparent. Decreases in <br />snowfall are noted when seeding the colder <br />equivalent potential temperatures. At warmer <br />equivalent potential temperatures the seeding effect <br />reverses and snowfall increases when seeding the <br />warmest stratifications are substantial. These <br />increases are significant at the 5% level for most <br />tests in the Climax I and Wolf Creek I samples. Both <br />the two-sample Wilcoxon test and the two-sample <br />sum of squared ranks test indicate significance at <br />the 10/0 level for the Wolf Creek I sample when <br />analyzed without control. <br /> <br />c. Stability and baroclinic considerations. <br />The stability of the air mass approach- <br />ing the mountain barrier may influence the modifica- <br />! tion potential in complex ways. If the air mass is <br />convectively unstable precipitation may tend to con- <br />: centrate in relatively small cells and convective lines. <br /> <br />The stronger upward motirn s in these cells and lines <br />would result in high supply rates of cloud water in <br />localized areas. However, the stronger upward <br />motions would also probably result in higher cloud <br />tops. Since the number of effective ice nuclei <br />increases exponentially with cloud top height, while <br />tl::e need for additional ice nuclei grows only directly <br />with the upward speed, it is not obvicu s that modifi- <br />cation potential would be greater in uIlstable air <br />masses. On the other hand, if the convective <br />stability is quite low (near zero) and modification <br />potential exists for other reasons (lack of available <br />ice nuclei, for existing c1cu d conditions), the additional <br />release of latent heat resulting from seeding might <br />generate precipitation of a convective nature that <br />would not otherwise have occurred. <br /> <br />The static stability cf the air mass <br />also affects the nature of the laminar flow over the <br /> <br />17 <br />