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<br />\ --- <br /> <br />of freedom are permitted to independently express the various ch,aracter- <br />istics of a surface raincell, namely shape, area, location of precipitation <br />maximum, and,in particular, precipitation gradient. <br /> <br />A model isohyetal pattern for a convective raincell is shown in Fig 2. The <br />spatial distribution of precipitation for such patterns is given by: <br /> <br />P(x) = PM [0.5 + 0.5 cos (~rx/ro)J G <br /> <br />(1 ) <br /> <br />where P(x) is the precipitation amount at point x; PM is the maximum <br />precipitation amount at point M (not necessarily at the geometrical center <br />of the pattern); rx is the distance from point M to point x; ro "is the <br />distance from point M to point 0 (on the zero isopleth) through point x; <br />and G is the spatial gradient index. The location of M is externally <br />defi ned by the parameters X Offset and Y Offset, the coord"i nate offset <br />distance ratios from the geomE~trical CE~nter of the pattern to thE~ zero <br />isopleth. The shape of the pattern is determined by the parametE~r E (labelled <br />Ellipse in Fig. 2) the ratio of major to minor axes of the elliptical <br />pattern. To faci 1 itate general ity of the results, the major axi s of the <br />isohyetal pattern (labelled LENGTH in Fig. 2) is arbitrarily scaled to always <br />be 16 km (10 mi) long. <br /> <br />Fig. 3 shows the relationship between G and ASO, the percentage of raincell <br />area containing 50 percent of the total precipitation volume (labelled half <br />area in Fig. 2). It can be seen that A50 is a nonlinear function of G. A <br />value of G equal to 0.6 (A50 = 25) corresponds to an approximately linear <br />spatial gradient of precipitation. Both parameters are carried throughout <br />the paper because A50 is an easily derived value from isohyetal maps and, <br /> <br />6 <br />