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Last modified
7/28/2009 2:39:45 PM
Creation date
4/23/2008 11:58:46 AM
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Weather Modification
Title
Snow Accumulation Algorithm for the WSR-88D Radar, Version 1
Date
6/1/1996
Weather Modification - Doc Type
Report
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<br />established between what a radar measures, Ze' and R, the rainfall accumulation, or S, the <br />snowfall accumulation. <br /> <br />Many studies have been published concerning Z-R relationships for rain, usually of the form <br />of equation (1) with the a and ~ ,coefficients empirically determined, using units of mm6 per <br />m3 for Z and mm h-l for R. For a variety of reasons involving microphysics, vertical air <br />motions and other factors, no unique relationship exists for either rain or snow. Progress has <br />been made in optimizing values of a and ~ for different types of rain and different <br />geographical regions. However, the CUITlmt practice with the network of WSR-88s is to use <br />a = 300 and ~ = 1.4 as the default values in equation (1) for rainfall estimation nationwide. <br /> <br />Less work has been done with Z-S relationships for snowfall. Reasons for more emphasis on <br />rain include greater importance of rainfall to society in general, and the increased difficulty <br />of detecting snowfall because of its generally lighter rates, typically producing melted water <br />equivalent values in the range less than 0.10 inch h-l. Such accumulations are well below <br />common rain accumulations, especially from convective storms. Therefore, snowfall requires <br />sensitive radars for detection at even modl~rate ranges. Moreover, because the signal-to-noise <br />ratio is often relatively low for snowfall intensities, and because snowfall often develops in <br />shallow clouds, ground clutter returns can more easily hinder attempts to quantify snowfall. <br /> <br />Discussing the merits of various ground dutter suppression schemes is beyond the scope of <br />this report. Section 3.3 discusses the diffil~ulties of not having an automatic electronic record <br />of how, when, and where ground clutter suppression was applied with WSR-88D radars. It <br />is certainly recommended that steps be taken to record suppression methods in use on future <br />Level II tapes. The general approach taken in development of this Algorithm has been to <br />attempt to measure S in areas around Cleveland and Denver which presumably have little <br />or no ground clutter, even when that approach meant locating snow measurements farther <br />from the radar than desired for development of Ze-S relationships. The alternative was to <br />measure S within areas shown to have potential ground returns by the clutter bypass maps. <br />This practice would result in Ze observations that may have been suppressed to unknown <br />degrees, depending on the radial wind speed, the degree of suppression applied (notch width <br />map setting), and other factors. That approach could only add unknown variance to <br />development of a Ze-S relationship because the "true" Ze could never be determined. <br /> <br />Two basic, but fundamentally different, approaches can be used to relate radar measurements <br />to precipitation in general, and snowfall in particular. With the'most common approach, the <br />reflectivity factor is calculated from surface observations of snow particles without <br />involvement of radar measurements. The definition of the reflectivity factor, Z, is the <br />summation of the sixth powers of melted drop diameters divided by the contributing volume <br />Vc; that is: <br /> <br />Z:=LD6/Vc <br /> <br />(2) <br /> <br />This approach has a number of problems, including uncertainties in the density and fall <br />speeds of individual snowflakes needed to estimate the volume each particle represents. <br />These uncertainties are especially acute when often-present aggregation and/or riming are <br />important to the snowfall progress. Snowflake densities and fall velocities are usually <br />. estimated from empirical functions with particle size, introducing the uncertainty of how <br />representative these functions are for the particular snowfall being sampled. . Another <br />problem is obtaining sufficient particle observations to be representative of the large volumes <br /> <br />19 <br />
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