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Last modified
7/28/2009 2:39:54 PM
Creation date
4/23/2008 12:04:05 PM
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Template:
Weather Modification
Contract/Permit #
87-1999
Title
Development of Empirical Equations of Ice Crystal Growth Microphysics for Modeling Analysis - Final Report
Date
9/1/1988
Weather Modification - Doc Type
Report
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<br />t <br /> <br />30 <br /> <br />. <br /> <br />growth environment is small with respect to the absolute temperature level <br />involved. Classical conduction and diffusion theories express the fluxes of <br />heat and water vapor between the environment and the outer boundary of <br />the resistance layer, and the transportations based on Knudsen's flow describe <br />the fluxes within the layer. Only parts of the heat and water vapor reaching <br />the particle surface through the resistance layer are conveyed to the ice <br />particle. Assuming the steady state fluxes and applying the appropriate <br />boundary conditions, the diffusion - kinetic equation, an expression <br />governing the rate of mass growth of the particle with respect to time under <br />the conditions mentioned above, becomes: <br /> <br />I <br /> <br />. <br /> <br />. <br /> <br />dm <br />dt = <br /> <br />41tr(Si - 1) <br />L2 l' <br />( 2 + ) <br />KRvT _fex P....,satDfy <br /> <br />(3.1) <br /> <br />. <br /> <br />where <br /> <br />. <br /> <br />fex=r I(r+ la), <br /> <br />(3.2) <br /> <br />f",/ = r I ( r + I)' ), <br /> <br />(3.3) <br /> <br />. <br /> <br />2aK(21tRa T 00)1/2 <br />la = (2 - a)p(cv + Ra/2) , <br /> <br />(3.4) <br /> <br />. <br /> <br />2yD ( 21t )1/2 <br />1",/ = R T <br />2-y voo ' <br /> <br />(3.5) <br /> <br />. <br /> <br />where m is the ice crystal mass, Si (= pool p 00, sat) the saturation ratio with <br />respect to ice , r the radius of the spherical ice particle, L the latent heat of <br />deposition, K the thermal conductivity, Rv specific gas constant for water <br /> <br />. <br />
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