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<br />15 <br /> <br />number density set by the melting rate of that hailstone. Thus, total mass continuity <br /> <br />is maintained while hailstones melt away in mass at constant number density to re- <br /> <br />appear as variable number densities of conserved mass raindrops. Any particles <br /> <br />formed too large for physically realistic raindrops are assumed to immediately break <br /> <br />up via the breakup term of Srivastava (1971). This process thus maximizes the <br /> <br />rate of transfer of hail mess to large raindrops and may tend to underestimate the <br /> <br />hail amounts reaching the ground in relation in total rainfall. <br /> <br />'" <br /> <br />Dynamics <br /> <br />General Framework <br /> <br />The cloud in this work is modeled as a radially symmetric cylindrical air <br /> <br />column with a time independent radius in an environment at rest. The pressure in <br /> <br />the column is assumed to adjust instantaneously at each level to that of the environment <br /> <br />which is assumed to be in a state of hydrostatic equilibrium. All equations are formu- <br /> <br />lated in one-climensional space in a manner similar to that of Asai (1962), Asai and <br /> <br />Kasahara (1967) and Ogura and Takahashi (1971) with respect to the dynamic terms. <br /> <br />The system of equations formulated in this work is that used by Nelson (1971) and <br /> <br />greatly expanded by Silverman and Glass (1973) to permit realistic simulation of <br /> <br />time dependent tropical warm cumulus clouds. This study will further expand the <br /> <br />dynamical framework and microphysical-dynamic interaction terms to allow for ice <br /> <br />and ice-processes and to thus permit the simulation of continental clouds in which <br /> <br />the ice phase may playa significant role in precipitation production. <br />