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<br />APRIL 1984 <br /> <br />SMITH ET AL. <br /> <br />503 <br /> <br />seeding would show up on the measuring instruments. <br />Determination of the persistence of the ice crystal <br />plumes generated by the seeding was also desired. <br />Therefore, measurements from successive cloud phys- <br />ics aircraft passes through the cloud at about 2 and 5 <br />min after treatment were included as response vari- <br />ables. Both aircraft and radar observations of the times <br />of first appearance of precipitation within the cloud <br />and below cloud base were specified. The aircraft ob- <br />servations were less ambiguous with regard to particle <br />sizes and concentrations, but the radar observations <br />provided a better view of the whole cloud volume. <br />Both radar and aircraft measurements of total rainfall <br />amounts were used, because neither was free of un- <br />certainties. <br />The order of the primary response variables in Table <br />3 differs from that presented in the design document <br />(Bureau of Reclamation, 1979). The original sequence <br />of "8-minute variables," A We8, PIC8, MVD8 was <br />rearranged to PIC8, MVD8, A WC8. In developing the <br />original experimental design, little thought was given <br />to the order of these variables because all three were <br />to be measured by the cloud physics aircraft during a <br />pass through the cloud about 8 min after treatment. <br />However, as part of the statistical evaluation of the <br />experiment, the response variables were introduced in <br />sequence, one at a time, into a multivariate analysis <br />(Mielke et al., 1984). There the order makes a differ- <br />ence, and the arrangement in Table 3 makes more <br />physical sense, in view of the experimental hypothesis, <br />than the original order. That is, the precipitating ice <br />particles were hypothesized to be responsible for de- <br />pletion of the cloud liquid water (as illustrated by Or- <br />ville and Chen, 1982). Therefore, either higher con- <br />centrations or larger sizes of precipitating ice particles, <br />or both, in seeded clouds should precede any difference <br />in the cloud liquid water concentration. (This reor- <br />dering was made only after the evaluation of the ex- <br />periment was underway. We do not claim that pro- <br />cedure to be above statistical suspicion, but believe it <br />is acceptable in this exploratory experiment. In any <br />case,. the main point is that the order of the variables <br />can be important when any sequential multivariate <br />analysis is planned.) <br />The scenario approach to the experimental design <br />mentioned in Section 2 can be illustrated with reference <br />to MVD8, the mean volume diameter of the precip- <br />itation-sized particles observed on the pass through the <br />cloud 8 min after treatment. For this and several other <br />variables, it was necessary to specify default values to <br />cover test cases for which there were no applicable <br />observations, because missing values cause great dif- <br />ficulties in multivariate analyses. The 2D-P instrument <br />used to measure the precipitation particle sizes yielded <br />data for 0.2-mm size increments, but the data were <br />. regarded as unreliable for the first size channel. More- <br />over, some definitions of "precipitating ice particles" <br />require a minimum size of at least 0.5 mm. Therefore, <br />the smallest acceptable size was set at 0.6 mm. <br /> <br />Suppose no particles 0.6 mm or larger were found <br />on the 8-min pass; what value should be assigned to <br />MVD8? One possibility would be to take MVD8 = O. <br />However, the experimental hypothesis (Table 2) in- <br />dicates that". . . in the seeded clouds. . . larger sizes <br />of (precipitating ice) particles are present at comparable <br />times after treatment." One can postulate a scenario <br />in which the particles in nonseeded clouds are, say, <br />0.4 mm in diameter, while those in the seeded clouds <br />are 0.6 mm in diameter (on that pass). According to <br />the rules, the observations of 0.4 mm particles would <br />be rejected, but taking the default value as zero would <br />clearly accentuate the difference between seeded and <br />non seeded clouds, an unsatisfactory effect because the <br />statistical evaluation procedure (Mielke et al., 1984) <br />operates essentially on the separation between seeded <br />and nonseeded cases. Because of the implications of <br />. this scenario, the default value for MVD8 was set at <br />0.6 mm. That, of course, might reduce the seed/no- <br />seed difference and so dilute the power of the exper- <br />iment, but that was regarded as the more acceptable <br />alternative. <br />One primary response variable originally defined <br />(RERA, a radar rainfall estimate that was to be adjusted <br />on the basis of one or more radar Z-R relationships <br />developed from the HIPLEX-I data) has not yet been <br />computed. To do so requires an analysis of raindrop <br />size data observed by the cloud physics aircraft during <br />the experiment to determine a Z-R relationship (or <br />perhaps more than one) specifically for the HIPLEX- <br />I test cases. The radar rainfall estimates, computed <br />using the resultant Z-R relationship(s), would pre- <br />sumably differ from RERC. The relevant data were <br />examined (Arnesen, 1982), but it has not been possible <br />to resolve all the issues encountered, within the effort <br />and time available. <br />Only the primary response variables are associated <br />directly with key elements of the physical hypothesis. <br />In this exploratory experiment it was also thought use- <br />ful to check several secondary response variables (Table <br />3) that might be influenced by the seeding. One sec- <br />ondary response variable OIiginally defined (MVDP, <br />the maximum mean volume diameter of the hydro- <br />meteors observed beneath the cloud) has not yet been <br />computed because of the time and effort involved. The <br />final test statistics reflect the ultimate goal of HIP LEX, <br />namely to develop technology for increasing the pro- <br />portion of clouds that precipitate and the amount of <br />precipitation per experimental unit. In a statistical <br />sense, the A VRA and A VRC statistics are redundant <br />with the primary response variables AER and RERC. <br />Related statistical hypotheses indicating the desired <br />or expected senses of the various responses were also <br />spelled out in the HIPLEX-I design document. In each <br />case, the null hypothesis was to be tested by permu- <br />tation methods. The multi-response permutation pro- <br />cedures (MRPP) described by Mielke et al. (1981) pro- <br />vided the principal test methods used. The expected <br />sense of the alternative, to be evaluated using point <br />