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<br />v . iN = o. <br /> <br />(3) <br /> <br />. <br /> <br />r . <br /> <br />The microphysics in the model uses bulk parameterizations for both the water and the <br />ice phase. The water phase is parameterized according to a moclliied form of the Kessler <br />(1969) scheme. This parameterization is described in detail in Clark (1979). In this scheme, <br />condensed ~ater exists in two forms, as cloud- and rainwater, with mixing ratios qc and <br />ca. The ice phase parameterization closely lollows the work ol Koenig and Murray (1976), <br />herea.:Cter ret'erred to as K-M (The ice phase parameterization will be discussed in more <br />detail in the next section). The K-M parameterization allows lor two types of particles, <br />ice crystals initially lormed by heterogeneous ice nucleation or ice splinter processes due to <br />riming (type A) and ice particles (graupel) initially formed by freezing of raindrops (type <br />B). Consequently nve categories, denoted by subscript j, lor the water substance have to be <br />taken into account in the equations for the conservation of heat, water and ice substance. <br />The categories are: <br />1. Water vapor <br /> <br />f" <br /> <br />r " <br /> <br />; <br />,- <br /> <br />,".. <br /> <br />\. .: <br /> <br />2. Suspended drops <br />3. Rain drops <br />4. Type A ice <br /> <br />. <br /> <br />\ <br />i .. <br /> <br />S. Type B ice <br /> <br />i <br />i <br />l,: <br /> <br />The equations governing heat and moisture conservation are <br /> <br />ro' <br />( . <br />f <br />i...... <br /> <br />-DS- pLt. (0 ) pLt. (0 ) pLi. (0 0 0) <br />P-D =---= 2d1 + ---= 3dJ + -= ;d1 + ;dJ + ". ;-4 5 <br />t OpT OpT OpT ' <br />+ ~~f (Od. - C;dl);.4,5 + ~f (0;dl)1-4.5 + V. (pKHVS-) <br /> <br />(4) <br /> <br />p~~. = -P(Oid1);.2.4., + 1 (0;dJ);aa.4., - pC". + v. (pKHVq.) (5) <br /> <br />. <br /> <br />29 <br />