Laserfiche WebLink
<br />792 <br /> <br />ABBS: r:;VESTIGATION OF PROBABLE MAXIMUM PRECIPITATION ASSUMPTIONS <br /> <br /> <br />(a) <br /> <br />150 <br /> <br /> <br />150 <br /> <br /> <br />150 <br /> <br />Figure 6. Plots of the percentage of the total rainfall that <br />falls as heavy rainfall (i.e., with a rainfall rate >25 mm h~l) for <br />(a) the control simulation. (b) EC86_3, and (c) EC86_5, The <br />re'tllt.< shown orc for grid 3. Black contours are for 10%, and <br />dark shading is for percentages >50%. <br /> <br />rainfall. For Ihe casc of the heavy rain[all. precipitation pro- <br />duction is 80%-90% efficient. As the amount of moisture <br />available to the system increases, there is a tendency for PEr to <br />decrease for moderate rainfall. The lower plots of Figures Sa. <br />5h, and 5c show that as the moisture available to the system is <br />increased, the number of heavy rainfall grid points increases <br />and the heavy rainfall is longer-lived, <br />The percentage of the total rainfall that occurs as heavy <br />rainfall has been calculated for the control simulation. <br />EC86_3, and EC86_S and is shown in Figure 6, For cach <br />simulation the rainfall that falls in the main cloud hand over <br />the sea occurs as heavy rainfall. Over the land, only a small <br />percentage falls as heavy rainfall, but this amount increases as <br />the moisture availability increases. Figures 5 and 6 indicate <br />that long-lived moderate rain processes are important and that <br />the efficiency of these processes may decrease as the moisture <br />availability increases. On the other hand, this may be offset by <br />increases in the percentage of rain falling as heavy rainfall. <br />3.2.4. Terrain effects. When estimating PMP values for a <br />particular storm, it is usual to attempt to separate out the <br />convergence and topographic components of the storm. The <br />concept underlying this technique is that the convergence com. <br />ponent is due to synoptic-scale atmospheric disturbances such <br />as frontal lifting. The portion of the rainfall that cannot be <br />separated into the convergence component is defined as the <br />topographic component of the storm. <br />In this section, results are presented for Q simullltion wllhnut <br />Ictrltln: thlli ltimuhulun mllY be considered to be the model <br />equivalent of the convergence component for this storm. The <br />convergence component rainfall is then subtracted from the <br />rainfall of the control simulation to provide an estimate of a <br />model-derived topographic component of this storm. The con. <br />vergence and topographic components of the storm are pre- <br />sented in Figure 7. <br />These results show that over the Blue Mount'.lins and IIIa- <br />warra escarpment almost all of the rainfall is due to the topo- <br />graphic component of the storm. However, along the conver- <br />gence line the results are more complicated. The removal of <br />terrain has allowed the entire system to move south faster than <br />in the case of the control simulation. Consequently, the rainfall <br />maximum of 267 mm, for the "no terrain case," occurs farther <br />south than the corresponding maximum of 355 mm for the <br />control simulation, The effect of this difference may be seen in <br />the adjacent, large maximum and minimum values of Figure <br />7b, A topographic component of -100 mm in this region is <br />more realistic. However, these results illustrate that terrain <br />effects do feed back to synoptic-scale aspects of the storm. <br />3.2.5. Depth~duration-area analysis. The model~derived <br />precipitation fields have been uscd to calculate DDA curves <br />for the control simulation, EC86_3, and EC86_S, These curves <br />are based on hourly rainfall rates for the finest mesh simulated <br />and calculated using the same method as Minty et ai, [1996]. <br />This melhod differs slightly from the standard method [WMO, <br />1969J in that multicentercd storms are trcated as if they werc <br />single-centered [Minty et ai" 1996. P, 8J: <br /> <br />I <br /> <br />I <br />I <br />I <br />, <br />\ <br />I <br />I <br />i <br /> <br />The program which determines maximum depth-area curve for <br />each storm simply cOllnts the numher of grid points in hctwccn <br />evenly incrcmented isohycts, from the maximum to the minimum <br />isohyct. and calculates the arithmetic mean rainfall per interval. <br />Area calculalions are based upon the number of grid points <br />counted and the known resolution of the grid. <br /> <br />In all cases the hourly rainfalls used in these analyses are <br />from 6 hours of simulation to the completion of the simulation. <br />