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Last modified
7/28/2009 2:40:09 PM
Creation date
4/23/2008 1:57:37 PM
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Weather Modification
Title
Microphysical Observations Over the Atlas Mountains in Morocco
Date
12/23/1988
Weather Modification - Doc Type
Report
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<br /> <br />l V2,q:!,02 <br />fAP2 <br /> <br />Zz <br /> <br />Vo,qo,Oo <br /> <br />} VI,q ,,0. <br />API <br /> <br />Z, <br /> <br /> <br />APO <br /> <br />Zo <br />Xo <br /> <br />X, <br /> <br />X2 <br /> <br />~: Symbolic two-dimensional flow <br />across a barrier. <br /> <br />1 [ t.n^ V^ <br />r (q + Qo) ~g <br />0,1 = Pwt.x 0 <br /> <br />~] <br />- (ql+Qd g <br /> <br />\. <br /> <br />where: <br /> <br />ro,], = average precipitation rate over <br />the distance t.x <br /> <br />q = layer mean water vapor specific <br />humi dity <br /> <br />Q = layer mean cloud water (liquid <br />or solid) specific humidity <br /> <br />t.p = layer thickness (in pressure <br />units) <br /> <br />v = mean horizontal velocity of <br />1 ayer <br /> <br />9 = gravity <br /> <br />Pw = density of water (1 g cm-3) <br /> <br />For two-dimensional, steady-state, <br />hydrostatic flow, the continuity equation <br />can be written (assuming water substance <br />changes negligible): <br /> <br />t.Po Vo = t.PIVl = t.P2V2 <br />--- <br />g g g <br /> <br />Therefore (2) can be written. in general <br /> <br />~[ <br />rl,I+l = (qI+QI) <br />pt.xg <br /> <br />(qI+l+QI+l)} <br /> <br />where <br /> <br />q dqs Ah <br />1+1 - qI = dz U 1,1+1 <br /> <br />dqs!dz was defined in (1) and t.hI 1+1 is <br />the parcel vertical displacement &etween <br />point 1 and 1+1 and t.hI.I+l can be written <br />as <br /> <br />t.hI,I+l = d(zI+l - II) <br /> <br />where <br /> <br />d = 1 - (1 - ~~:)G~ = ~n <br /> <br />is the vertical displacement factor <br />depending on the degree of stability and <br />moisture of the parcel. <br /> <br />If we define: <br /> <br />( 2) <br /> <br />qI - qI+l = t.CI.I+1 (5) <br /> <br />as condensation per unit mass. occurring as <br />the parcel moves from point I to point 1+1. <br />and specify that a constant fraction E of <br />the sum of condensate formed and "imported" <br />precipitates over t.x. the remaining cloud <br />water, QI+l at point 1+1 is: <br /> <br />QI+l = (I-E)QI + (I-E)t.CI,I+l (6) <br /> <br />Now, substituting (5) and (6) into (2) <br />yields: <br /> <br />- Vot.Po [ 1 <br />rI.I+1 = Pw(gt.x)E QI + t.CI.I+1 (7) <br /> <br /> <br />The term [QI + t.CI 1+1] can be either <br />>0 (condensation) 'or < 0 (evaporation). <br />In the latter case. rI.I+l = o. <br /> <br />The model uses. as input: <br /> <br />. Rawinsonde data analyzed and <br />interpolated for 15 evenly <br />spaced pressure layers. <br /> <br />. A fine mesh topography grid of <br />35 x 45 points with t.X = 10.0 km <br />(see Fig. 2). <br /> <br />. The stations' coordinates for <br />which estimates of precipitation <br />are to be made. <br /> <br />( 3) <br /> <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />(4) <br /> <br />I · <br />- <br />. <br />~. <br />... <br />C1 <br /> <br />. <br /> <br />Fir. 2: Model topography obtained using <br />a 0 km grid interval. <br />
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