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Last modified
7/28/2009 2:33:46 PM
Creation date
3/20/2008 1:07:52 PM
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Template:
Weather Modification
Title
Observations and Numerical Simulations of Precipitation Mechanisms in Natural and Seeded Convective Clouds
Prepared By
Lroen D. Nelson
Date
3/1/1979
State
IL
Weather Modification - Doc Type
Report
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<br />30 <br /> <br />A potentially more serious model pseudodiffusion error may occur due to <br /> <br />the use of a variant of upstream differencing (see Kovetz and Olund, 1969), for <br /> <br />particulate mass advection (condensation/sublimation). In this model, condensation/ <br /> <br />sublimation is done in series with the other parallel model processes to permit the <br /> <br />continued recalculation of a maximally large U d~t/~ via a separate cClnden- <br />con <br /> <br />sational At, thus minimizing pseudodiffusive errors in particulate mass growl'h. Since <br /> <br />the J and K scale particulate spacings ore far apart in mass at larger sizes, it might <br /> <br />be thought that the numerical diffusion errors in condensation would become! quite <br /> <br />large at larger sizes. Fortunately, this effect is offset by the rapid decreasE~ with <br /> <br />particle size of the effective condensation driving force. <br /> <br />Because of the complicating effects of the nonlinear mass scale and '~he non- <br /> <br />constant advective velocity (mass condensation rate) involved in numerical solution <br /> <br />of the condensation equation by the upstream difference technique, the moss <br /> <br />pseudodiffusion effect of the numerical scheme is not easily solved for analytically. <br /> <br />Silverman and Gloss (1973) have investigated this problem in detail by a series of <br /> <br />model runs using different numbers (mass spacings) of hydrometeor mass classE~s. They <br /> <br />conclude that 45 log scale mass classes to cover the hydrometeor size spectrum (as <br /> <br />is done in this model for both ice and liquid particles) leads to reasonable and <br /> <br />stable results while models using appreciably fewer size classes will be subject to <br /> <br />significant particle size pseudodiffusion errors. <br /> <br />As a check on the applicability of their conclusions to this larger model in- <br /> <br />c1uding ice phase effects, the model simulation of the August 14, 1975 Big Spring <br /> <br />Texas Cloud (given later as Table 4 and Figures 20 through 26) was repeated with <br />
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