Laserfiche WebLink
<br />per kilometer) is proportional to the <br />product of the mass, weighted hydrom, <br />eteor axis ratio and the precipitation <br />liquid water content (Jameson 1985), <br />and is derived from the range derivative <br />of the differential propagation phase <br />between vertically and horizontally po- <br />larized radiation, Also, KDP tends to in, <br />crease from 00 km-1 to several degrees <br />per kilometer in regions of substantial <br />precipitation liquid water content. <br />Qualitatively, LDR provides informa- <br />tion on the hydrometeor phase, shape, <br />and orientation by measuring the relative <br />amount of depolarized power (in dB) re- <br />turned from scatterers in a given radar <br />pulse volume, Pulse volumes with mix, <br />tures ofliquid water and ice (e,g" mixed <br />phase) or canted, irregularly shaped par, <br />ticles all act to increase the LDR. In the <br />case of the FCL flood, ZDR' KDP' and LDR <br />were collected by the CSU-CHILL ra- <br />dar and when combined with reflectiv- <br />ity and CG lightning data, provide <br />insight into the microphysical character, <br />istics of the flood convection, <br />To set the framework for discussion <br />of the polarimetric observations, first <br />consider the time-height series of KCYS <br />mean radar reflectivity computed for a <br />stationary cylindrical volume (lO,km <br />radius, l4-km height) centered on Taft <br />Hill and Drake Roads in FCL, shown in <br />Fig, 15 (28 July 19971725-2225 MDT), <br />Note that Fig. 15 also includes a time <br />series of rain mass flux (CSU-CHILL <br />radar estimate; see section 7d) and marks <br />indicating the time of occurrence of in- <br />dividual CG lightning flashes, Three pri- <br />mary pulses in convective rainfall <br />separated in time by approximately 1- <br />1.5 h are apparent in Fig, 15 (peaks at <br />minutes 85, 155, 260), The life cycle of <br /> <br />FIG. 12. Dual~Doppler-derived horizontal <br />wind vectors (m 5-1) and radar reflectivity (shaded) <br />for the l,km height level at (a) 2110 MDT 28 July <br />1997 and (b) 2130 MDT 28 July 1997. Grid ori- <br />gin as in Fig. 9. Vector scale (m 5-1) is indicated <br />in the upper-right comer. <br /> <br />Bulletin of the American Meteorological Society <br /> <br />. <br /> <br /> nO <br /> 40 <br />~ <br />. <br />~ <br />e 20 <br />Q <br />'E <br />; <br />" <br />, 0 <br />... <br />E <br />.s <br />~ -20 <br />z. <br />. <br />- <br />c <br />~ -40 <br /> -nO <br /> <br />C 40 <br />.. <br /> <br />. <br />-;! <br />~ 20 <br /> <br />'C <br />C <br />, <br />" <br />, <br />l- <br />E <br />2 <br />~ <br />:r, -20 <br />i. <br />. <br />i; <br />~ <br />is --40 <br /> <br />a, 2KJULY 1997,2IHl MDT: dIl7JH-WI:'\D (Z=I KM) <br /> <br />'-I " , , <br />20 30 40 45 50 <br />'0 <br /> <br />--7 I' <br /> <br /> <br />-xo <br />,40 <br /> <br />.20 <br /> <br />20 <br /> <br />40 <br /> <br />K<' <br /> <br />100 <br /> <br />120 <br /> <br />o <br /> <br />nO <br /> <br />Distance E.W from Taft and nrakt' (km) <br /> <br />b, 28 JULY 19')7,2130 MDT: dIl7JH-WIND (Z=I KM) <br /> <br />'--I , , , <br />20 30 40 45 50 <br /> <br />", <br /> <br />--7 IS <br /> <br />00 <br /> <br /> <br />o <br /> <br />'\ <br /> <br />.60 <br /> <br />~ <br /> <br />o 20 40 6U ~U <br /> <br />I(J() <br /> <br />120 <br /> <br />,so <br />-40 <br /> <br />-20 <br /> <br />Dlstau\'e f:'W from Taft and Drake (kntl <br /> <br />205 <br /> <br />- <br />