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<br />TABLE III. --Estimate of 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 a computed vertical gradient of potential condensate <br />in the 700-500 mb layer. <br /> <br />( <br /> <br /> With Controls Without Controls <br /> Total Sample Scale Scale <br />Stra tifica tion Sample Size Change Change <br />GM/O:<GM)(100 mb) Size Utilized Method (0/0) P- Value (0/0) P- Value <br />Climax I <br />o to < O. 7 S 24 S 24 NPl -36 .058 < -50 .0045 <br /> NS 21 NS 21 NP2 -46 .0314 < -50 .0071 <br /> (S17, NS19) PAR -40 .072 <br />0, 7 to < 1. 3 S 76 S 76 NPl +4 . 371 +11 .284 <br /> NS 86 NS 86 NP2 +6 .334 +8 .274 <br /> (S6l, NS66) PAR +3 .401 <br />1. 3 to < 2. 0 S 20 S 20 NPl +117 .0351 +53 .154 <br /> NS 24 NS 24 NP2 +171 .147 +100 .145 ~I <br /> (S12, NS17) PAR +128 .0150 <br /> <br />S 15 S 15 NPl -38 .147 < -50 .049 <br />NS 12 NS 12 NP2 <-50 .0239 < -50 .0336 <br /> (S10, NS11) PAR -45 .134 <br />S 36 S 36 NPl +7 .341 + 5 .397 <br />NS 42 NS 42 NP2 -5 .452 +16 . 212 <br /> (S31, NS34) PAR +2 .468 <br />S 10 S 10 NPl >+200 .0239 >+200 .0392 <br />NS 12 NS 12 NP2 >+200 .082 >+200 . 142 <br /> (S8, NS8) PAR +145 .090 <br /> <br />Climax II <br /> <br />o to < O. 7 <br /> <br />O. 7 to < 1. 3. <br /> <br />1. 3 to < 2. 0 <br /> <br />Wolf Creek Summit <br />o to < O. 8 S 33 S 30 NPl -21 .184 -20 . 187 <br /> NS 38 NS 34 NP2 -39 .074 --24 . 102 <br /> (S10, NS25) PAR -10 .238 <br />O. 8 to < 1. 2 S 58 S 55 NPl +11 .394 -14 .370 <br /> NS 81 NS 80 NP2 +2 .448 -15 .284 <br /> (S36, NS53) 'PAR +20 .149 <br />1. 2 to < 2.0 S 73 S 62 NP1 +128 .0202 >+200 .0025 <br /> NS 79 NS 67 NP2 >+200 .0021 >+200 .0012 <br /> (1lI40, NS43) pAR +-65' .0094 <br /> <br />mountain barrier. This is apparent from the <br />influence the static stability term exerts in the wave <br />equatiffi s for flow over mountain barriers as <br />discussed by Scorer (1953). Thus, the static stability <br />helps to determine the orographically induced <br />vertical motion field over the mountain barrier. The <br />integrated effect of stability upon modification poten- <br />tial is therefore difficult to assess. <br /> <br />The distribution of seeding effects <br />with a convective stability index is shown in Table V. <br />The three independent samples are in agreement in <br />most respects. All three samples indicate snowfall <br />decreases when seeding the most stable categories. <br />The two Climax samples show snowfall increases <br />when seeding the most unstable events (less than <br />1. 0) and again in an intermediate range (4.0 to 8.0). <br />This double mode in evidence at Climax is not <br />repeated at Wolf Creek Summit, but instead a gradual <br /> <br />decr~~s(i; ~n positive seeding effects with increasing <br />stablhty lS noted. The increase in snowfall when <br />seeding the unstable events is significant at the 5% <br />level for some afth~ tests for Climax I and Wolf Creek <br />I samples. <br /> <br />The mean temperature advection in the 700- <br />500 mb layer has been computed and provides a <br />measure of the baroclinic state of the atmo sphere. <br />The distribution of seeding effects with the mean <br />temperature advection in the clou'd layer is shown in <br />Table VI. The three samples are again quite con- <br />sistent. It is seen that snowfall increases are <br />observed when seeding the moderate baroclinic <br />conditions (warm or cold advection), The snowfall <br />increases at Climax are spectacular when seeding <br />the moderate warm advection events. All tests <br />indicate significance at the 5% level in the Climax I <br />sample. <br /> <br />18 <br />