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<br />, <br />I <br />I <br />, <br />I <br />I <br />I <br />J <br />i <br />j <br />~ <br />j <br />I <br />1 <br />I <br />I <br />I <br />, <br />i <br />1 <br />, <br />1 <br /> <br />i <br />I <br />I <br />j <br />I <br />I <br /> <br />ABBS: INVESTIGATION OF PROBABLE MAXIMUM PRECIPITATION ASSUMPTIONS <br /> <br />convective parameterization scheme on the finest grid to ini~ <br />tiate convective development in locations dose to those ob. <br />served. For those cases the 7 km grid is too coarse to resolve <br />adequately the vertical motion scales most important to the <br />simulations. In these simulations the convective scheme is <br />phased out as the convection matures, following the method- <br />ology of Chen and Frank [1993]. Wang and Seaman [19971 <br />discuss the use of a convective parameterization scheme for <br />simulations with a grid spacing of the order of 10 km and <br />report their findings for a number of case studies and several <br />convective parameterization schemes. They found that it is not <br />appropriate to use the explicit moisture scheme alone at these <br />model resolutions and that there were significant advantages to <br />using a convective parameterization scheme that directly rep- <br />resented moist, convective downdrafts. <br /> <br />3.2. East Coast Low: August 4-6 <br /> <br />3.2.1 Validation. The model simulation commenced at <br />1200 UTC on August 4 and was run for the next 36 hours, <br />finishing at 0000 UTC August 6. The ECMWF mean-sea-Ievel <br />pressure analyses have been compared with the mean sea level <br />pre~sures predicted by the model for 0000 and 1200 UTC on <br />August 5 and 0000 UTC on August 6 (not shown). This com- <br />parison showed the rapid decrease in central pressure of the <br />low between 0000 and 1200 UTC and the close agreement <br />between the modeled and ECMWF pressures. At both of these <br />times the modeled pressures were within 2 hPa of the ECMWF <br />pressures, At 0000 UTC on August 6, there is less agreement <br />between the model and ECMWF analyses. with the model <br />beginning to increase the central pressure of the low and the <br />ECMWF analyses. indicating little change in the central pres- <br />sure of the low. It is believed that this erroneous 7 hPa pressure <br />rise is related to the prediction of the convection on the finest <br />mesh, as the rise does not occur in simulations with two levels <br />of grid nesling, Bolh the ECMWF analyses and the model <br />predictions show little horizontal movement of the low <br />throughout the final 24-hour period. <br />Figure 2 compares the observations of 0500 UTC, August 5, <br />with the model predictions corresponding to this time of the <br />wind field at the lowest model level (50 m) and the mean sea <br />level pressure. The features to note are the strong convergence <br />of the low-level winds at the leading edge (i.e., south of the <br />center) of the low and the weak winds that occur inland and <br />north of the low center. At this time. the modeled central <br />pressure of 1004 hPa compares favorably with the observed of <br />1002 hPa. The main difference between the model-predicted <br />and observed fields is that the model positions the low -60 km <br />further north and further offshore than the observed. <br />These discrepancies in the position of the low are reflected <br />in the precipitation predicted by the model. Figure 3 shows the <br />24-hour precipitation. ending at 2300 UTC on August 5. for <br />the observations and the model prediction. Both show a band <br />of heavy precipitation, of -300 mm, extending inland to the <br />Blue Mountains. The major difference between the two fields <br />is that the model predicts the band of heavy rainfall to occur <br />farther north than is observed, In addition, the northern <br />boundary of the rainfall band occurs farther north in the model <br />prediction. The orographic effect of both the Blue Mountains <br />nntJ the IIIawurru cscarpmcnt Is obvious in the local maxima in <br />the precipitation over both of these regions. As in the obser. <br />vations {Bureau of Meteor%gy, 1987J. the maximum rainfall <br />lies to the west of the lIIawarra escarpment and along the <br />southern escarpment of the Blue Mountains. The predicted <br /> <br />I <br />l <br />, <br />j <br /> <br />7SlJ <br /> <br /> <br /> <br />30 <br /> <br />3S <br /> <br />I <br /> <br />14S 150 155 <br /> <br />Figure 2. (a) Regional mean sea level pressure analysis <br />(hPa) at 05lHl UTC, August 5 [from Bureau of Meteorolo!.'Y. <br />1987] and (b) simulated regional mean sca level pressure anal- <br />ysis (hPa) at 0500 UTC, August 5, Results shown are for grid <br />2. Shading indicates terrain higher than 250 m with a contour <br />interval of 500 m. <br /> <br />rainfall amounts over both the Blue Mountains and the IIIa- <br />warra escarpment are very close to those observed. Inh:l1sily~ <br />frequency-duration curves (not shown) have been calculated <br />for this simulation. These indicate that the model has been <br />able to capture the extreme intensity of the 8-hollr duratiun <br />precipitation. <br />When considering the quality of the model prediction, it <br />must be kept in mind that these predictions have bet:n pro- <br />duced at a horizontal resolution of -7 km from initial conJi. <br />tions that are available at a resolulion of - 250 km. Overall, the <br />model has predicted a realistic development of the cast coast <br />low and the predicted precipitation amounts and intensities ar~ <br />close to the extreme values observed. ConlicqUl,mtly, WI.: h~lil,;v~ <br />that this simulation provides an adequate test for many uf the <br />assumptions made in the estimation of PMP values. <br />3.2.2. Increased moisture simulations. The simulations <br />discussed in this section have been performed by initializing <br />