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<br />510 <br /> <br />JOURNAL OF CLIMATE AND APPLIED METEOROLOGY <br /> <br />VOLUME 23 <br /> <br />permitted by increased understanding, leading ulti- <br />mately to an area seeding experiment. <br />2) A detailed multistep physical hypothesis was for- <br />mulated with emphasis on the expected differences <br />between seeded and nonseeded clouds. For each step <br />of the hypothesis, response variables compatible with <br />, the measurement capabilities available for the exper- <br />iment were defined, so that the expected differences <br />could be monitored. For the response variables asso- <br />ciated with each step, indications were provided of <br />how (at least implicitly), when, and where the seeded/ <br />nonseeded differences were to be measured. This aspect <br />of the experimental design is important because it pro- <br />vides for determining not only whether the seeding <br />produces increased rainfall, but also whether the phys- <br />ical mechanism is correctly understood. <br />3) Physical measurements of the characteristics of <br />candidate clouds were made and analyzed in real-time <br />to determine their suitability as experimental units. <br /> <br />Because of the approach that was used, HIPLEX- <br />I has been able to make a meaningful contribution to <br />the undet;"Standing of precipitation processes (natural <br />and modified) in cumulus clouds in spite of the un- <br />timely termination of the experiment and the small <br />sample size that resulted. HIPLEX-I was a test of <br />"static" seeding with dry ice, carried out to produce <br />microphysical effects in the clouds. The use of dry ice <br />permitted timely introduction of the ice nucleating <br />agent into the desired regions of the clouds, and ver- <br />ification of the production of ice crystal plumes by the <br />seeding was included in the experiment. The physical <br />and statistical evaluations of HIPLEX -I will indicate <br />the degree to which the physical hypothesis describes <br />the actual precipitation processes in the test case clouds. <br /> <br />Acknowledgments. We wish to acknowledge the <br />contribution of Richard Eddy in compiling the HI- <br />PLEX-I design document. Glenn Brier also contrib- <br />uted to the experimental design. Dr. Sumedha Sen- <br />gupta prepared the randomization sequences, and Jack <br />McPartland supervised their execution in the field. The <br />Learjet seeding aircraft was furnished and operated by <br />Colorado International Corporation, while the Uni- <br />versity of Wyoming provided the King Air cloud phys- <br />ics aircraft. The successful conduct of HIPLEX-I is <br />due in considerable measure to the accomplishments <br />of these two organizations in developing the equipment <br />and operating procedures for the project aircraft. A <br />special acknowledgment goes to the many unnamed <br />members of the HIPLEX-I field crews, whose dedi- <br />cation and competence helped make the conduct of <br />the experiment a success. Barbara Brown was the an- <br />alyst who "boxed" the radar echoes as described in <br />Section 7; she, John Middleton, and David Priegnitz <br />carried out the computations of the radar response <br />variables. We are grateful to Paul Lawson for supplying <br />Figs. 2, 3, and 4. <br /> <br />Preparation of this manuscript was supported by <br />the Division of Atmospheric Resources Research, Bu- ' <br />reau of Reclamation, U.S. Department of the Interior, <br />under Contract 8-07-83-Y0009. <br /> <br />APPENDIX <br /> <br />Synopsis of Procedures for Calculating Primary <br />Response Variables <br /> <br />In specifying the locations from which data were <br />taken to determine the aircraft response variables, three <br />navigational "pointers" were used. They were defined <br />as follows: <br /> <br />Pointer I: The location where the maximum cloud <br />liquid water concentration was observed on the pre:- <br />treatment pass. <br />Pointer 2: The location within a cloud where the <br />maximum ice-crystal concen~ration was observed on <br />the first pass after treatment (2-min pass). <br />Pointer 3: The location of the center of the precip- <br />itation shaft as first encountered at the + 100C level. <br /> <br />Each pointer provided a floating frame of reference, <br />in which integrating the displacements determined <br />from the aircraft heading and true airspeed to zero <br />brought the aircraft back to the same point in the air <br />(that is, drifted with the environmental wind). On the <br />passes from two to about 17 min after treatment, the <br />cloud physics aircraft attempted to return through the <br />location of Pointer I. Thereafter it attempted on each <br />pass beneath the cloud to go through (in order of prioJr- <br />ity): the center of a radar echo, if one appeared; the <br />center of the visible rain shaft, if any; Pointer 3 aft(~r <br />it had been set during a pass through the rain shaft <br />beneath the cloud, which subsequently disappeared; <br />or the vertical projection of Pointer I. Pointer 2 was <br />used to determine when to expose a decelerator slide <br />on the cloud penetration about 5 min after treatment. <br />The flight path segments specified for computing <br />each variable were based on estimates of the diffusion <br />of the seeding plume that are discussed in Appendix <br />D of Bureau of Reclamation (1979), with allowanc(:s <br />for possible displacement of the seeding track from <br />the path of the cloud physics aircraft on the pre-treat- <br />ment pass and for wind shear between flight levels. To <br />make the definitions of the response variables fully <br />objective, default values were specified to cover situ- <br />ations where the measurements did not produce a value <br />of a particular response variable in accordance with <br />the established criteria. The default values were chosen <br />so that they would tend either to have no effect 011, <br />or to reduce, the separation between seeded and non- <br />seeded cases in the MRPP analysis. The individual <br />variables were calculated as follows: <br /> <br />CIC2: The average number concentration of ice <br />crystals observed by the Particle Measuring Systems <br />(PMS) 2D-C probe (depolarization channel) during a <br /> <br />~ <br />