<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
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