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<br />". <br /> <br />co <br /> <br />I <br />V <br /> <br />Before discussing the results of the <br />model comparison with observations, several points <br />concerning this phase of the workshop need to be <br />emphasized. First, it should be recognized that <br />the data sets were not collected for this purpose <br />and are, therefore, not as appropriate as they <br />might need to be. The second point is that model <br />runs were necessarily limited by the available <br />input data and program run costs, an expense <br />which was borne by the sponsors of the partici- <br />pating modelers. Considering the sensitivity of <br />model results to input conditions, this is an <br />important point to remember when examining the <br />comparative predictions. Lastly, it should be <br />remembered that a major purpose of this model <br />comparison was to lay the foundation for designing <br />a more explicit and meaningful model-observation <br />experiment that would be conducted in the future. <br /> <br />Tables 2 and 3 give results of the <br />various model runs for clouds which fit into <br />approximately the size of the observed clouds for <br />that day, except for the slab-symmetric models <br />which predict their own size clouds. Table 2 is <br />for August 10 and table 3 is for August 17. In <br />general, the one-dimensional, steady-state models <br />or single parcel Lagrangian models, which are <br />models 1 through 3, predict the taller clouds <br />observed on the days. Their maximum vrrtical <br />velocities ranged from 15 to 25 m sec-. Note <br />the different results for model I (la and lb of <br />tables 2 and 3). These two sets of results show <br />the model's sensitivity to different initiating <br />impulses of 2 and 1 m sec-l, respectively. This <br />further illustrates the importance of proper <br />model initialization. In general, all of the <br />parameters for each of the three models showed the <br />proper tendency when compared with observations. <br />That is, the parameter differences tended to be <br />of the same sign, though not necessarily of the <br />same magnitude, as the observed differences <br />be~veen August 10 and 17. The rainfall accumu- <br />lations from these lD, SS models were not con- <br />sidered'to be a realistic prediction and were <br />not taken very seriously by the modelers at the <br />conference. <br /> <br />,<::,~' ,O>~. <br /> <br />,,' <br />," <br /> <br />,,' <br />,.. <br /> <br />,,' <br />,+; <br /> <br />,oA~' <br /> <br />". <br />J" <br /> <br />100. <br /> <br />..J'..J~"'.J-..,f..J'J'~~~~Y <br /> <br /> <br /> <br />~. ~~fi~~~~~~~~':: <br /> <br /> <br /> <br />9Q / ..~t .. / ',' t., ',.", ,', / <br /> <br />300. <>~:5t~:~.:~;:>~~;:~~:~:.::;:~~~:~;~ "'", <br /> <br />~oo. .-,- .....--f-.---\~.-r-~ -.--.~__....L..;.o..-~.L--4..~~ ... <br />~;~. >< ....... ~~..~:... V(.....~<~;.~~~.>;<\........(......~. . ?,()' <br />500. ~-/-::J-x/ ;r.~<L~~~7' ;:L"-;'-!--'v"c"", './..' ~". <br />,,'.. ' '.' '. . ". /, ". \ ". '. ' <br />600 %-7':' --':', - ',,-:: -"+7"'-\.."~P-'--.:)...-L'':::' '::-'... <br />., ~"" ...... .~ ~..<;;,.)~.. ,''-'>}'l.1 ....< \ ....1. ......;1./.... <;/1.<:;)' <br />700. -,......;- - . .;--,-t;; _ .;k--3....;~~-a.-,~\2'-.:;-'~r ""':.- <br /> <br />:gg:~7~'" .::~... ':-:Z;;";.~:~.~~~~~~;;.::::.?!:~ <br /> <br />1000. . . . I. . <br /> <br />STL811 <br />INIT1AL SOUNDING AT 13 HR 0 HIN <br />Fi(JW'e 2. Skew-T analysis showing terrperatu:r>e and <br />dewpoint profiles for St. Louis, Mo., on August l7, <br />Z073. at lJOO L.S.T. <br /> <br />~~L_~____,-"<-_ <br /> <br />The one-dimensional, time-dependent <br />(lD, TD) models numbered for the 10th, of. . <br />which three gave fairly realistic results. For <br />August 17, there were five runs made with one- <br />dimensional, time-dependent models. In general, <br />the one-dimensional, time-dependent models gave <br />lower cloud tops than the steady-state models. <br />The bases were predicted by these models and, in <br />some cases, checked out fairly well, and in all <br />cases within one grid interval of observed <br />cloud base. Maximum vertical velocities for these <br />models on August 10 ranged from 16 to 19.8 m sec~l <br />and on August 17 from 11.4 to 21.5 m sec-l. The <br />rain rates on August 10 were up to 54 rom hr-l, <br />which agreed well with the observations for that <br />size cloud. Rainfall accumulated on the ground in <br />these models was, in general, less than observed. <br />Two of these models did predict hail at the ground, <br />which was observed, and most of the models <br />predicted the right tendency, at least partly. <br /> <br />The two-dimensional, time-depeudent <br />(2D, TD) slab models predicted a field of clouds <br />and were successful in predicting the proper <br />tendency from the 10th to the 17th. In addition, <br />the cloud tops, vertical velocity maximum" maximum <br />rain rate, and maximum accumulated rainfall were <br />within the range of the observations. Neither of <br />these models predicted significant hail at the <br />ground, although one of them does include a hail <br />process. <br /> <br />t >-- <br />t <br /> <br />~.r'A <br />. . <br /> <br />:/' -"-~,~': <br />I I I <br />20 30 40 <br />TIME <br />AUGUST 17, 1973 <br /> <br />I <br />'" <br /> <br />I <br />" <br /> <br />I <br /><0' <br /> <br /> <br />\ <br /> <br />,1 <br />I <br />I <br />I <br />I <br />I <br />/.-f\--r...., <br />, . <br />~. <br /> <br />_......1.--..J <br />" " <br /> <br />TIME <br />AUGUST 10. 1973 <br />OBSERVED RAOAR ECHO TOPS '1$. TIME -NEAR ST. LOUIS, MISSI)URI <br /> <br />Fi(JW'e 3. Corrparison between observed radar echo- <br />top height (solid lines) and predicted time-height <br />cross section (dashed) from three modeZs for <br />August lO and l7, 1973. Note the similar' <br />characteristics of models and observations. <br /> <br />~ <br />