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<br />a. <br /> <br />KCYS: 28 July 19971730-2225 MDT <br />I 1-1-, ,-I~Uil'~ <br />1 2 3 3,5 4 4,5 5 5.5 <br /> <br />10 <br /> <br /> <br />~ <br />~ 5 <br />~ <br />" <br />.:.:: <br />" <br />.... <br />Q <br />"0 0 <br />= <br />'" <br /><::: <br />'" <br />Eo< <br />~ -5 <br />rf) <br />i <br /> <br />/ <br />, <br />, <br />, <br />I <br />I <br />I <br />, <br />I <br />J. <br />-,. <br />I <br />I <br />I <br />, <br />\ <br />, <br />I <br />I <br />I <br /> <br />I <br />I <br />I <br />/ <br />/ <br /> <br />I <br />\ <br />, <br /> <br /> <br />I <br />I <br />I <br /> <br />I <br /> <br />-10 <br />-10 <br /> <br /> <br />-5 0 5 <br />E-W of Taft and Drake (KM) <br /> <br />b. <br /> <br />CHILL: 28 July 1997 1730-2215 MDT <br />1 [-'1-, , I<',r-r~ 1 <br />1 2 3 4 5 6 6,5 7 7.5 8 <br /> <br />10 <br /> <br /> <br />~ <br />::;: <br />~ <br />~ <br />" <br />.:.:: <br />'" <br />.... <br />Q <br />"0 <br />= <br />'" <br /><::: <br />'" <br />Eo< <br />"'" <br />o <br />rf) <br />i <br /> <br /> <br />5 <br /> <br />~ <br /> <br />o <br /> <br />, <br />, <br />I <br />I <br />I <br />I <br />.( ~ <br />--.. <br />1 ( <br />I <br />l- <br />I <br />, I <br />.,.' I <br />/ <br />, <br /> <br />, <br />,\ <br />-- <br /> <br />-5 <br /> <br />10 <br /> <br />-10 <br />-10 <br /> <br />10 <br /> <br />-5 0 5 <br />E- W of Taft and Drake (KM) <br /> <br />FIG, 19, Storm,total rainfall (in,), 1725-2215 MDT 28 July 1997, (a) NEXRAD Z-R estimate using KeyS reflectivity data, (b) <br />CSU-CHILL blended R(Kop, ZOR) estimate. The contour interval in (a) and (b) is 1 in. The origin ("0") is located as in Fig. 9. FeL <br />street grid and location of Spring Creek are also depicted as in Fig. 9. Note the change in scale for shading of rainfall amounts in (a) <br />and (b), <br /> <br />standard errors of the estimators reported in Bringi <br />et aL (1996) for the CSU-CHlLL radar, The "tropi, <br />cal" Z-R rela1ionships shown in Table 2 (Short et aL <br />1997; Rosenfeld et aL 1993) were utilized in the <br />blended product (Fig, 19b), Sensitivity tests suggest <br />that the blended product was relatively insensitive to <br />the tropical Z-R relationship used and also to small <br />changes (e,g" 0,10 km-', 0,1 dB, I dBZ) in the Kop' ZOR' <br />and reflectivity thresholds chosen, Relative to the <br />R(Kop, ZVR) estimate, the blended rainfall product (Fig, <br />19b) exhibited a slight decrease (7%) in the maximum <br />STP, but smoother (spatially) instantaneous rain rates, <br />In summary, the NEXRAD Z-R relationship ap' <br />plied to both KCYS and CSU-CHILL radar reflectiv- <br />ity data produced STP maxima that were only <br />50%-65% of the gauge STP maximum (similar to un- <br />derestimates of rainfall by the NEXRAD in the Madi- <br />son County, Virginia, flash flood of 1995; Smith et al. <br />1996), While good agreement was attained between <br />gauge-measured STPs and STPs computed using the <br />(Short et aL 1997) Rosenfeld et aL (1993) tropical <br />Z-R relationship with the (CSU-CHILL) KCYS <br />NEXRAD data, the relative degree of agreement be, <br />tween the Z-R,computed STP and the gauges was <br />clearly a function of both the radar and relationship <br /> <br />212 <br /> <br />. <br /> <br />used (Table 2), This is not surprising given the strong <br />functional dependence of Z-R,computed rain rates on <br />sampling error, radar calibration, and variations in the <br />drop size distribution (cf, Doviak and Zmic 1993), <br />A previously published R(K"p' ZOR) relationship <br />applied to the data in both pure and blended forms <br />(e,g" combined with the COARE tropical Z-R) pro, <br />vided a reasonable estimate of the STP with minimal <br />tuning (low by a factor of 0,8), It is hypothesized that <br />the combined phase and power information contained <br />in the R(Kop, ZOR) estimate better accounted for spa- <br />tial and temporal variations in the raindrop size dis, <br />tribution (e,g" Ryzhkov and Zmic 1995), <br /> <br />8. Summary <br /> <br />Extensive meteorological sampling of the environ, <br />mem, convection, and heavy rainfall associated with <br />the Fort Collins flash flood provided key insights into <br />the physical processes responsible for the flood event. <br />From a meteorological perspective the Fort Collins <br />case occurred under the influence of many classic syn- <br />optic signatures (e,g" Maddox et al. 1978; Maddox <br />et al. 1980; Caracena et al. 1979; Doswell et aL 1996), <br /> <br />Vol. 80, No.2, February 1999 <br />