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Last modified
7/28/2009 2:40:04 PM
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4/23/2008 1:56:56 PM
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Weather Modification
Title
The Evolution of Raindrop Spectra in Warm-Based Convective Storms as Observed and Numerically Modeled
Date
12/12/1978
Weather Modification - Doc Type
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<br />DECEMBER 1978 <br /> <br />R. E. CARBONE AND LOREN D. NELSON <br /> <br />2313 <br /> <br />large. The authors would not anticipate: that specifics <br />of the results herein could be successfully applied to <br />different environmental condiitions or storm types. <br /> <br />8. Conclusions <br /> <br />'. ';I <br /> <br />Radar and aircraft observations together with one- <br />dimensional, time-dependent model simulations have <br />revealed the following characteristics of convective <br />storms in Texas: <br /> <br />1) During July and August early echoes are usually <br />the result of warm rain processes. <br />2) On the intensively studied days where storms pro- <br />duced large quantities of precipitation, early echoes' <br />resulted from both liquid and ice phase processes. <br />3) Drop-size distributions at cloud base show sys- <br />tematic variability in time and space. <br />4) Temporal evolution is dominated by updraft <br />sorting (sedimentation) effects where small drops do <br />not have sufficient terminal velocity to fall through <br />cloud base. The result is a high number density of <br />drops > 3 mm diameter and a low number density of <br />drops < 2 mm diameter during the cloud growth stage. <br />During this stage number densities are typically one <br />order of magnitude lower than MP values at the 1 mm <br />diameter size. <br />. 5) During the dissipation stage drop spectra assume <br />MP characteristics in the model. The observations, <br />while evolving toward the MP form, rarely achieve <br />comparably high concentrations of small drops or <br />comparably low concentrations of large drops. <br />6) Model runs including and excluding the collision <br />breakup process suggest that collision breakup is not <br />important at and below cloud base when prior updraft <br />sorting has drastically reduced the total number con- <br />centration of drops. <br />7) Close agreement in observed and modeled <br />spectral form has been shown with the numerical <br />results of Srivastava (1971, 1978). These results suggest <br />that the spontaneous breakup process may be important <br />for rainfall rates ~ 30 mm h-1 and liquid water content <br />~ 1 g m-3. <br />9) The high variability of drop spectra precludes <br />the reliable use of conventional radar (Z-R) rainfall <br />estimation techniques in convective precipitation unless <br />some allowance for spatial and temporal change is <br />made. <br /> <br />The principal limitations of this investigation are <br />related to sample volume considerations in the observa- <br />tions and one-dimensionality of the model. To achieve <br />temporal stratification of the data, it was necessary to <br />average data over a finite path length in space. To <br />discern spatial variations, it was necessary to average <br />data in time. Updraft sorting, while clearly evident in <br />the model, may be an artifice of one-dimensionality. <br />Consideration of alternative explanations to updraft <br />sorting requires a two-dimensional model, such that <br /> <br /> <br />rain is not necessarily forced to fall through an updraft. . <br />The authors propose that future numerical work should <br />address the situation where rainfall rate is ~ 30 mm <br />h-1 and liquid water content is ~ 1 g-3 'to tully evaluate <br />the importance of various physical processes. In <br />particular, the question arises as to whether an en- <br />semble of drops will evolve to a unique equilibrium if <br />given enough time. The findings of this investigation <br />cast doubt on the concept of a unique equilibrium in <br />the presence of strong vertical air motions. Conse- <br />quently, the authors strongly encourage further <br />numerical work on the- effects of sedimentation. <br />Acknowledgments. The authors are indebted to Mr. <br />Donald Takeuchi for the processing of aircraft data <br />and to Mssrs. S. Howard, R. L. Reace, Jr., and D. <br />Suder for processing of radar data. Dr. Eugene Mueller <br />and Mr. Mark Gardner provided valuable assistance <br />with respect to digitization of radar data. Professor <br />R. C. Srivastava, Dr. T. B. Smith and Dr. Bernard <br />Silverman are gratefully acknowledged for stimulating <br />discussions and helpful suggestions. Ms. Gail Rust <br />performed typing and editing of the manuscript <br />admirably. <br />This research has been supported in part at <br />Meteorology Research, Incorporated, under contracts <br />from the Bureau of Reclamation and the Texas Water <br />Development Board. The National Center for Atmo- <br />spheric Research is sponsored by the National Science <br />Foundation and operated by the University Corporation <br />for Atmospheric Research. <br /> <br />APPENDIX <br /> <br />Model Changes and Differences from the <br />Warm Cloud Model of Silverman <br />and Glass (1973) <br /> <br />. Ice hydrometeors have been added to the model. <br />All ice is assumed spherical with adensityofO.9g cm-3. <br />. There are 45 liquid and 45 ice hydrometeor classes <br />in this model. <br />. Ice is formed in the model by nucleation from the <br />vapor and drop freezing. <br />. Riming is computed via a stochastic collection model <br />assuming the same collection efficiencies as used for <br />liquid coalescence. <br />. All liquid touching ice freezes to ice. No wet growth <br />of hail is allowed. No ice multiplication process <br />is allowed. <br />. Ice phase effects have been incorporated in the <br />thermodynamic, motion and continuity equations. <br /> <br />REFERENCES <br /> <br />Alusa, Alexander L., 1975: The role of drop breakup in the <br />development of raindrop-size distributions. J. Recl1. Almas., <br />9, 1-10. <br />Asai, T., and A. Kasahara, 1967: A theoretical study of the <br />compensating downward motions associated with cumulus <br />clouds. J. Almos. Sci., 24, 487-596. <br /> <br />
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