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<br />'0 <br /> <br />28 JULY 1997 NLDN <br />JIJ1}7.1I7,28 IK.2.'\ MDT r\EG = 1.315 POS = W9 <br /> <br /> <br />"" <br /> <br />40 <br /> <br />g <br />" <br />~ <br />~ <br />C <br />" <br />;; <br /> <br />:w <br /> <br />-tf+ <br />;:'1- <br /> <br />,- <br />" <br />.... <br />E <br />= <br />.: <br />:r.. -20 <br />i <br />t <br />c <br />~ -40 <br /> <br />o <br /> <br />= <br /> <br />-60 <br /> <br />- <br /> <br />-1\0 <br />-40 <br /> <br />-rl <br />." <br /> <br />-20 <br /> <br />o <br /> <br />20 <br /> <br />4{) <br /> <br />60 <br /> <br />I>islam't' E.\\' fmlll Taft and I>rukt'" (kill) <br /> <br />'0 <br /> <br />100 <br /> <br />120 <br /> <br />wind and rain mass flux after 2030 MDT, <br />consistent with the hypothesis that local <br />enhancements in the easterly wind re, <br />suIted in a corresponding increase in <br />heavy rainfall over FCL Caracena et al. <br />(1979) noted a similar correlation be, <br />tween changes in the easterly flow and <br />corresponding changes in rainfall for the <br />BT flood, <br />The resultant quasi, stationary nature <br />of the storm during the last 1.5 h of the <br />event appeared to be the result of an in, <br />crease in the magnitude of the system <br />propagation vector, which, in the net, ex- <br />tended toward the south,southwest. The <br />appearance of new cells and heavy rain <br />along the southern flank of the storm was <br />likely the result of interaction between <br />the enhanced, moist east-southeasterly <br />flow, a weak low-level outflow bound- <br />ary (Fig, 10), and local topography <br />(Fig, 2), Hence, the sum of cell move- <br />ment and system propagation vectors <br />resulted in a quasi, stationary storm (e,g" <br />Miller 1978; Chappell 1986), <br /> <br />FIG. 11. Cloud-ta-ground lightning detected between 1800 and 2300 MDT on <br />28 July 1997. Grid origin as in Fig. 9. Colors represents CO flash locations de- <br />tecLed in I,h intervals, J 800-1900 (btue), t 900-2000 (purple), 2000-2tOO (green), <br />2100-2200 (red), and 2200-2300 MDT (black), The locations of negative and <br />positive polarity CO flashes are indicated by a (-) and (+), respectively. The CO <br />flash 'counts by polarity are indicated in the upper-right comer of the figure. The <br />small box embedded within the larger grid encloses the area plotted in Fig. 9. <br /> <br />Radar reflectivity data (Figs, 9d-i) indicate that the <br />last group of convective cells and heavy rainfall be, <br />gan 10 stall over southwestern FCL after 2030 MDT, <br />nearly coincident with the onset of increased low,level <br />east,southeasterly flow. To further illustrate the rela, <br />tionship between the increased easterly wind compo, <br />nent and the onset of heavy convective rainfall after <br />2030 MDT, a time series (2032-2215 MDT) of line- <br />averaged easterly wind speeds and the relative devia- <br />tion of those speeds from the value at 2032 MDT was <br />computed utilizing the dual, Doppler analyses, The <br />mean easterly wind components were computed along <br />a 25 km long north-south,oriented line, located at x <br />= 15 and extending from y = 10-15 in Fig, 12, The <br />relative deviation and mean of the easterly wind com- <br />ponent for each time was then overlaid on a time se, <br />ries of rain mass flux for the FCL storm computed <br />from CSU-CHILL polarimetric radar data (cf, section <br />7d), The resultant time series (Fig, 14) exhibits a high <br />positive correlation (r = 0,91) between the easterly <br /> <br />204 <br /> <br />r- <br /> <br />-""'--.........-~- <br /> <br />c, Combined polarimetric and <br />NEXRAD observations of stonn <br />vertical structure <br />Observations of deep convection us' <br />ing dual-polarized radar have provided <br />new insights into the microphysical and electrical de, <br />velopment of convective clouds (e,g" Goodman et at <br />1988; Bringi et aL 1997; Jameson et aL 1996; <br />Ramachandran et aL 1996; Carey and Rutledge 1996, <br />1998), Combinations of multiparameter variables such <br />as differential reflectivity (ZOR)' specific differential <br />phase (KDI')' and linear depolarization ratio (LDR) pro, <br />vide information on hydrometeor size, shape, and ther- <br />modynamic phase (the presence of oblate raindrops, <br />hail, melting, etc,; cf, Jameson and Johnson 1990; <br />Doviak and Zmic 1993), thereby reducing the ambi, <br />guities involved with inferring cloud microphysical <br />properties based solely on radar reflectivity (2), <br />For example, ZOR is the ratio (expressed in dB) of <br />reflectivity measured at horizontal polarization (ZH) <br />to that of vertical polarization and provides informa, <br />tion on the reflectivity' weighted mean hydrometeor <br />axis ratio, The presence of large, oblate particles (e,g" <br />large raindrops) tends to increase the ZnR from near <br />zero to several decibels, The Kol' (expressed in degrees <br /> <br />Vol, 80, No, 2, February 1999 <br />