Laserfiche WebLink
<br />,(. <br />, <br /> <br />II. .1; : <br /> <br />"' <br />~ <br /> <br />j" <br />o <br />- <br /> <br /> <br />- <br />~'jl <br />10 <br />* - <br />* <br />~"" <br />u <br />-.... <br /> <br />..................... <br /> <br />. <br /> <br />6 <br /> <br />.. <br />I <br />o <br />- <br />100 <br /> <br />tOl <br />R (MM/HR) <br /> <br />102 <br /> <br />Figure IlIA <br /> <br />relationships of buildin~ and decaying rain shafts <br />in this data set, which was gathered in a very <br />warm, wet sounding with a cloudbase temperature <br />of 16 .C. <br /> <br />From the data in figure IV we can deduce the mean <br />Z-R relations: <br /> <br />Z . 763Rl.365 <br />Z . 400Rl.560 <br /> <br />(early) <br />(late) <br /> <br />(3) <br />(.4) <br /> <br />The corresponding model';'predicted Z-R relationships <br />show the same relation to each other but to a mu.;h <br />larger extent, as given below: <br /> <br />Z . 89l2RO.875 <br />Z . l77Rl.375 <br /> <br />(early) <br />(late) <br /> <br />(li) <br />(tl) <br /> <br />Thus, the model \~ould associate an "early" 3D-dB:: <br />echo with a rain rate of 0.1 mm/hr and a "late" <br />30-dBz echo with a rain rate of 3.50 mm/hr. The <br />mean observational Z-R relations would predict the <br />rain shafts at 30 dBz to be 1.2 mm/hr (early) and <br />1. 8 mm/hr (late). If we use extreme rather than <br />mean values of A and Bfrom fi~ure IV, then the <br />rain rates predicted at a constnnt 30 dBz become <br />0.7 mm/hr (early) and 2.6 mm/hr (late). <br /> <br />3. CONCLUS IONS <br /> <br />The one-dimensional model which has inadequate <br />horizontal mixing and wind-shear overpredicts the <br />temporal evolution of the Z-R relation and, of <br />course, cannot address the spatial variations at <br />all. Nevertheless, sampled rain shafts confirm <br />that the temporal evolution predicted by the model <br />does indeed exist in the real world. The implica- <br />tions for rainfall estimation by radar (where only <br />. the sixth moment of the drop-size distribution is' <br />knolon) are profound in that the observed variabil,. <br />ity of the drop-size distribution is somewhat sys.. <br />tematic in both time and space. Thus, different <br />Z-R relations apply at different times and loca- <br />tions within the same rainshaft. While aircraft <br />sampling-vol~~e considerations do not permit com- <br />plete separation of these spatial and temporal <br /> <br />N <br />o <br />- <br /> <br />o <br />o <br />- <br />* <br />C'J toO <br /> <br />tol <br />R (MM/HR) <br /> <br />102 <br /> <br />Figure I1IB <br /> <br />'variations, it is clear that they do exist and <br />should be considered before making use of radar <br />:reflectivity to estimate convective rainfall rates. <br />rn practice this would be quite cumberso~e but not <br />:impossible to execute, since information as to the <br />llge of the rain shaft and position relative to <br />4~nvironmental winds is known to some extent. <br /> <br />!f the effect of a seeding treatment were to <br />jlncrease the duration of the mature stage of a rain <br />lihaft with respect to the duration of the building <br />litage, then the rainfall calculated with a constant <br />~:-R relation from radar data would underoredict the <br />!ieeding effect. On the other hand, a "paired" <br />c:loud experiment where the unseeded cloud tended <br />t:o be sampled later in its life cycle could easily <br />s;how 100 percent seeding effects where in fact none <br /> <br />o <br />(IJ <br /> <br />co <br /> <br />\0 <br />CO . . <br />D D O' <br />"1' D <br /> D <br /> D <br /> D <br />N <br /> D <br /> D <br />0 <br /> I <br />0,0 500. 0 1000 ' 0 1500 . 0 <br /> A <br /> Figure IV <br />