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<br />- 70 - <br /> <br />For heavy rains (> 25mm) the gaging requirements of Table 3 will <br />be red~ced (i:e. lesser density) somewhat and for light rains (< 2.5 mmO <br />they w1ll be 1ncreased (i.e. more gages per unit area). Although cautipn <br />should be exercised in extrapolating these estimates to other geograph-' <br />ical areas and weather regimes, they do provide a rough estimate of the' <br />measurement problem one might face in conducting a weather modification <br />experiment. . <br /> <br />3.2 Radar Estimation of Precipitation <br /> <br />Background <br /> <br />Weather radar is rece1v1ng increased attention in weather modi- <br />fication experiments, especially so, now that a computer processing <br />capability is a reality at many radar installations. Besides precipitaJ <br />tion detection and estimation, radar can be used to measure the vertical <br />and lateral extent of convective storms, their movemement and growth rate, <br />reflectivity profiles and, more recently, inf~rences of air motion can be <br />made with Doppler radars. <br /> <br />Radar is especially attractive for the estimation of precipita- <br />tion. In terms of rain detection, radar provides the equivalent of an : <br />infinitely dense raingage network which would make it a near perfect toql <br />for a convective precipitation measurement if the magnitude of the radar <br />precipitation estimates were without error. Unfortunately, this is fre- <br />quently not the case. Unless calibrated frequently, radar calibration is <br />always an uncertainty to some extent and the radar beam is usually not <br />uniformly filled with precipitation. Furthermore, the relationship of ; <br />radar reflectivity (2) to rainfall rate (R) is variable between storms ~nd <br />within storms even in the same geographical location and season (Stout and <br />Mueller, 1968, Joss et aI, 1968). One can also not count on "normal" re- <br />fractive conditions; with anomalous propagation, there is false echo and, <br />uncertainty as to what is being measured. All of these considerations <br />produce error in the radar estimation of rainfall. <br /> <br />Rather than attempt a quantitative correction for calibration <br />and beam filling uncertainties, anomalous propagations and Z-R variability, <br />it now appears more practical in many instances to calibrate the radar <br />against a few raingages. Radar defines the spatial variability and pro-I <br />vides a first estimate of the magnitude of the precipitation and the cali- <br />brating gages allow for its adjustment (Wilson, 1970). This still remaips <br />a rather controversial procedure. Several schemes (e.g. Brandes, 1975) : <br />have been proposed to accomplish the adjustment; our simplistic method , <br />used in Florida will be described briefly here. For a comprehensive dis~ <br />cuss ion of the use of radar in weather modification and other research, l <br />the radar is referred to a review paper by Atlas (1968) and to the lectures <br />by Melnichuk and Chernikov at the workshops. <br /> <br />Unadjusted Radar Performance in Florida <br /> <br />The radar systems and the methods of data processing in Florida <br />are described in some detail by Woodley et al (1975). Only the results <br />of the research will be described here. <br /> <br />~ <br /> <br />Radar performance in estimating Florida convective rains was <br />determined by making comparisons of gage and radar-derived volumetric <br />rainfalls for gage clusters. In 1972, 40 recording raingages were in- <br />