Laserfiche WebLink
<br />C~CI <br /> <br />,.,. <br />>10 , <br /> <br />o <br /> <br />IMPLICATIONS OF TI~rn DEPENDENT CONVECTIVE Z-R RELATIONS <br />FOR RADAR PRECIPITATION ANALYSIS <br /> <br />Loren D. Nelson <br /> <br />Bureau of Reclamation <br />Denver, CiOlorado <br /> <br />Richard E. Carbone <br /> <br />anI! <br /> <br />National Center for Atmospheric Research. <br />Boulder, Colorado <br /> <br />1. - INTRODUCTION <br /> <br />Most area-wide convective precipitation enhance:ment <br />experiments rely upon radar for estimating total <br />precipitation over the treatment area, because high <br />spatial resolution using conventional rain gauges <br />is prohibitively expensive. The accuracy of this <br />radar precipitation measurement is deoendent on the <br />applicability of the reflectivity-rainfall (Z-R') <br />relation assumed for the calculation of rain rate. <br /> <br />During the summer of 1975, radar, aircraft, and <br />surface observations of convective showers were <br />conducted as part of the High Plains Coonerativl, <br />Experiment (HIPLEX). The observations reoorted <br />here are selected results from the Texas-HIPLEX <br />site located in the Big Spring-Snyder area, whic:h <br />is approximately 150 km south of Lubbock in wes': <br />Texas. <br /> <br />Numerical simulations (Nelson) with a time- <br />dependent, one-dimensional microphysical Eulerilm <br />numerical model and cloud microphysical r.leasure.. <br />ments (Carbone) for an intensively studied stonl <br />(Big Spring, Texas, August 14, 1975) both show non- <br />standard and time-denendent Z-R relations throul'h- <br />out the storm's rainfall history. The nwnericaf <br />model used is described by Nels~n (1976). An ear- <br />lier version of the model without ice-phase micro- <br />physi~s has been discussed by Silverman and Gla!.s <br />(1973). The synoptic situation and field measure- <br />ments are given in more detail by Carbone et al. <br />(1976). A more detailed model-observation comp~ir- <br />ison is being prepared for publication. In thi!. <br />brief note we wish to concentrate only u~on the <br />model-predicted and field-observed nonstandard <br />time and space-dependent raindrop spectra and <br />reSUlting Z-R relationships and to co~ent upon <br />their implications for radar precipitation <br />analysis. <br /> <br />2. MODEL RESULTS AND FIELD OBSERVATIONS <br /> <br />We find the developing rainshaft to be character- <br />ized by high concentrations of large drops with <br />respect to conventional Marshall-Palmer (~I-P) <br /> <br />· The National Center for Atmospheric Research <br />is operated by the National Science Foundation. <br /> <br />distributions. The decaying rain shaft tends to <br />approach conventional M-P'behavior. This is illus- <br />trated by figures IA and IB which show the temporal <br />evolution of the parameters N(O) [cm-4J and <br />Lambda [em] in the exponential (~larshall-Palmer <br />type) raindrop size distribution given by Eq.(l). <br /> <br />N(D)-N(O) exp(-Lambda D) <br /> <br />(1) <br /> <br />Strai~ht solid lines in figure I represent the <br />classical ~-P values. Connected boxes represent <br />model predictions at times in minutes ~iven by the <br />numbers adjoinin~ the boxes. Dashed lines repre- <br />sent objectively smoothed estimates of the mean and <br />mean !l standard deviation of N(O) and Lambda in <br />rain cells sampled by the aircraft before reaching <br />their peak reflectivity on ground-based radar. <br />Chain-dashed lines are analogous values in decaying <br />rainshafts having passed their peak reflectivity. <br />About 4800 7-second running average estimates of <br />the parameters N(O) and Lambda versus aircraft- <br />measured cloudbase rainrate derived from a Particle <br />Measuring Systems Precipitation Probe are involved <br />in the "early" data, while the "late" data repre- <br />sent about 1140 estimates of these parameters. The <br />model predicts that N(O) can be two orders of mag- <br />nitude lower than the M-P value in develooing rain- <br />shafts,'while Lambda begins one order of ~agnitude <br />deficient. As the rainfall intensity builds, the <br />intercept (N(O)) increases while the slope remains <br />constant, a behavior opposite to the Marshall- <br />Palmer distribution. As the rainshaft decays, the <br />model-predicted behavior in both N(O) and Lambda is <br />adequately described by the ~larshall-Palmer distri- <br />bution (fig. I). The excess of large drops in the <br />early sta~es of the model rainshaft comes about <br />predominately by size sorting in the time-dependent <br />updraft, large drops ~eing ahle to fall down to the <br />cloudbase through the uodraft earlier than small <br />drops. As the precipitation-enhanced downdraft <br />develops, this vertical sorting becomes less impor- <br />tant and the drop spectra become more classical. <br />As seen in figure I, the observations in decaying <br />rainshafts (dotted lines) are (based on the !l <br />standard deviation lines) drawn from a distinctly <br />different pooulation than the developing rains haft <br />values. While these "late" observations show the <br />same trend as the model outout, they never approach <br />the M-P values as the model predicts. Figure II <br />shows sample spectra taken from the aircraft data <br />