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<br />502 <br /> <br />JOURNAL OF CLIMATE AND APPLIED METEOROLOGY <br /> <br />VOLUME 23 <br /> <br />TABLE 2: HIPLEX-L physical hypothesis. <br /> <br />For the seeded clouds, the sequence of events leading to the changes <br />in the precipitation characteristics of the clouds is hypothesized to <br />be as follows (response variables and final test statistics associated <br />with each step of the hypothesis are indicated in parentheses and <br />are defined further in Table 3): <br /> <br />I) An average ice-crystal concentration of about 10 L -I is produced <br />in the supercooled water cloud at temperatures higher than -100C. <br />The initial ice-crystal concentration in the unmixed seeding plume <br />will be considerably higher to allow for the effects of diffusion. The <br />average ice-crystal concentration produced by seeding in these warmer <br />cloud regions is higher than found in unseeded clouds at comparable <br />times after treatment.* (CIC2, CIC5) <br /> <br />2) Ice crystals grow by diffusion to a size where riming occurs, <br />so that higher concentrations of rimed crystals appear in seeded <br />clouds at comparable times after treatment. The seeding-produced <br />crystals tend to develop as columns. Crystals found at these tem- <br />peratures in unseeded clouds at comparable times after treatment <br />tend to have habits characteristic of growth at lower temperatures. <br />(CCR5, FCC5) <br /> <br />3) Rimed ice crystals in the liquid portions of the cloud grow by <br />accretion to graupel on the order of I mm in diameter and in con- <br />centrations of about 0.1 L -1, which then fall through the cioud. <br />Accretional crystal growth is accompanied by a decrease, relative to <br />the unseeded clouds at comparable times after treatment, in liquid <br />water concentration. The ice crystals produced by seeding have a <br />significant advantage over those that occur in unseeded clouds because <br />they originate earlier, in the lifetime of the cloud. This leads to the <br />earlier appearance of precipitating ice particles in the seeded clouds, <br />so, that greater concentrations and larger sizes of such particles are <br />present at comparable times after treatment. (PIC8, MVD8, A WC8, <br />TFPI) <br /> <br />4) Radar first echoes develop earlier in seeded clouds than in <br />unseeded clouds. (TFE) <br /> <br />5) Precipitation falls from cloud base in the form of graupel and/ <br />or rain (melted graupel) earlier in the lifetime of the seeded cloud <br />and in greater volume than occurs in unseeded clouds. In addition, <br />a larger proportion of seeded clouds than unseeded clouds will produce <br />rain. (TlPA, TlPR, TIPB, RERC, AER, A VRA, A VRC, PCPA, <br />PCPR) <br /> <br />6) Rain at the ground, averaged per experimental unit, is greater <br />for seeded clouds than for unseeded clouds. (No measurements of <br />rain at the ground are available for HIPLEX-I.) <br /> <br />* "Treatment" refers to the release of seeding material from the <br />seeding aircraft (in which case the cloud is seeded) or the activation <br />of a placebo mechanism (resulting in an unseeded cloud). <br /> <br />crease both the probability and the amount of precip- <br />itation from the test case clouds. <br />The statement of the physical hypothesis in Table <br />2 describes the expected sequence of events with em- <br />phasis on differences between seeded and nonseeded <br />clouds. Those differences are expressed in a form com- <br />patible with the measurement capabilities available for <br />the experiment. Elements in a hypothesis that are. not <br />subject to verification in the experiment, like Step 6 <br />of the HIPLEX-I hypothesis, are of little substantive <br />value in the experimental design. (It was recognized <br />at the outset that no feasible raingage network would <br />be able to measure the rainfall from the HIPLEX-I <br />clouds, because they were so small.) No hypothesis <br />was spelled out for the Class B clouds, because there <br /> <br />were uncertainties about the possible effects ofic~ mul- <br />tiplication or dynamic processes. It was expected that <br />the essential elements of the hypothesis in Table 2 <br />would probably also be valid for Class B clouds. <br />For each step in the physical hypothesis, one or <br />more response variable was defined and measured to <br />monitor the progress of the cloud behavior in com- <br />parison to that hypothesized. Table 3 contains a list <br />of the response variables for HIPLEX-l. The defini- <br />tions of the variables generally indicate when they were <br />measured; the locations of the measurements are dis- <br />cussed in the following section and in the Appendix. <br />Some degree of redundancy exists in the list of re- <br />sponse variables. For example, CIC2 and CIC5 both <br />indicate the ice-particle concentrations shortly after <br />the treatment time. There was some uncertainty about <br />just when the increased concentrations due to dry-ice <br /> <br />TABLE 3. Primary and secondary response variables and final test <br />statistics. <br /> <br />I CIC2 <br />2 CIC5 <br />3 CCR5 <br />4 PIC8 <br />5 MVD8 <br />6 AWC8 <br />7 TFPI <br />8 TFE <br />9a TIPA <br />9b TIPR <br />lOa RERC <br />lOb AER <br /> <br />Primary response variables: <br /> <br />Cloud ice concentration, 2 min after treatment <br />Cloud ice concentration, 5 min after treatment <br />Concentration of crystals rimed, 5 min after <br />treatment <br />Precipitating iCe number concentration, 8 min <br />after treatment <br />Mean volume diameter of precipitating ice <br />particles, 8 min after treatment <br />Average liquid water concentration, 8 min after <br />treatment <br />Time to first precipitating ice (particles with <br />diameters ~ 0.6 mm in concentrations> 0.1 <br />L-') <br />Time to first SWR-75 radar echo (15 dBz) <br />Time to initial precipitation at + 100C level, <br />aircraft measurement <br />Time to initial precipitation at + 100C level, <br />SWR-75 radar (15 dBz) <br />Radar-estimated rainfall at + 100C level, using a <br />constant Z-R relationship <br />Aircraft-estimated rainfall at + 100C level <br /> <br />FCC5 <br /> <br />Secondary response variables: <br /> <br />2 M2EA <br />3 M3EA <br />4 D2EC <br />5 D3EC <br />6 MAXZ, <br />7 TIPB <br /> <br />Final test statistics: <br /> <br />la PCPA <br /> <br />I b PCPR <br /> <br />2a A VRA <br /> <br />2b A VRC <br /> <br />Fraction of crystals which are columnar, 5 min <br />after treatment <br />Maximum area of the 20-dBz echo <br />Maximum area of the 30-dBz echo <br />Time duration of the 20-dBz echo <br />Time duration of the 30-dBz echo <br />Maximum radar reflectivity factor <br />Time to initial precipitation at cloud base (15- <br />dBz echo on SWR-75 radar) <br /> <br />Proportion of experimental units that precipitate, <br />based on TIPA <br />Proportion of experimental units that precipitate, <br />based on TIPR <br />A verage volume of precipitation per experimental <br />unit, based on AER <br />A verage volume of precipitation per experimental <br />unit, based on RERC <br />