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<br />6 <br /> <br />of the cloud. While there are many such microphysical Eulerian models in the <br /> <br />literature, the concepts involved in the Eulerian framework are typified by the <br /> <br />work of Nelson (1971) and Silverman and Glass (1973). <br /> <br />Since this model contemplates both detailed microphysics and microphysical- <br /> <br />dynamical interactions between various parts of a cloud, the numerical framework <br /> <br />used herein will be exclusively Eulerian. Chapter II will first describe the physical <br /> <br />equations of the simulated processes and then transform these differential-int(!gral <br /> <br />equations into the framework of Eulerian finite-difference iterative solution algorithms. <br /> <br />The microphysical processes and interactions to be simulated are illustrated schematically <br /> <br />in Figure 1 and have been selected to be a computationally manageable subset of the <br /> <br />larger diagram given by Braham (1968). <br /> <br />Microphysics <br /> <br />Condensation <br /> <br />The condensation growth of droplets containing dissolved hygroscopic: nuclei <br /> <br />is given by Silverman and Kunkel (1970) and Silverman (1972) as: <br /> <br />· dX . <br />x = - = x(x,y'P ,1') = 4,rrD'Fp H <br />at v s <br /> <br /> <br />I <br /> <br />1 + 20- <br />....odrTRv <br /> <br />(1 + S) (1 + S/2) <br /> <br /> <br />(eq. 1) <br /> <br />[1 + 2~ 1 <br />Ps PdrTRv <br /> <br />(1 +S)!(1 +S/2)R T2KlF' <br />v <br /> <br /> <br />* <br /> <br /> <br />-1 <br />