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Last modified
7/28/2009 2:32:24 PM
Creation date
4/11/2008 3:39:40 PM
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Weather Modification
Title
Application of a Simple Local-Scale Numerical Model in the Study of Altered Climate Impacts on Watershed Precipitation
Prepared By
J. G. Medina
Date
1/1/1989
State
AZ
Weather Modification - Doc Type
Report
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<br />;. <br /> <br />,^ <br /> <br />t <br /> <br />APPLICATION OF A SIMPLE LOCAL-SCALE NUMERICAL MODEL IN TIlE STUDY <br />OF ALTERED CLIMATE IMP Acrs ON WATERSHED PRECIPITATION <br /> <br />J. G. Medina <br />U.S. Department of the Interior <br />Bureau of Reclamation <br />Denver, Colorado U.S.A <br /> <br />1. INTRODUCTION <br /> <br />Prospects of global climate changes over the <br />next few decades have led to enhanced interest in <br />climate modeling. The Bureau of Reclamation <br />operates numerous water storage facilities and <br />hydroelectric dams and thus is concerned about <br />climate change effects that may occur on the scale of a <br />watershed. <br /> <br />Hydrological processes can amplify the effects <br />of altered precipitation that may occur from climate <br />changes. Consequently, there is substantial interest in <br />the study of effects on the local scale of 5 to 50 kIn. <br />Currently available general circulation models <br />(GCM's) utilize grid scales on the order of 200 to <br />400 kIn (e.g., Washington and Meehl, 1989). <br />Regional-scale models developed for climate studies <br />employ scales on the order of 50 to 100 kIn (e.g., <br />Giorgi and Bates, 1989). While the regional-scale <br />models substantially improve the description of effects <br />of features such as mountain chains over the GCM's, <br />there remains the need to study precipitation at the <br />watershed scale in order to study climate change <br />scenarios on, for example, reselVoir management. <br /> <br />This paper discusses the application of a <br />simple local-scale model to two geographically and <br />meteorologically very different areas to diagnose <br />winter precipitation on the scale of a watershed. <br />Specifically, the model is separately adapted to the <br />Delaware River watershed and the Mogollon Rim of <br />Arizona. Additionally, in the case of the Mogollon <br />Rim, input sounding data required by the model are <br />obtained from sites that are part of the national <br />rawinsonde network and, in a separate study, from <br />output from the Pennsylvania State University / <br />National Center for Atmospheric Research regional <br />meteorological model (MM4) (Anthes and Warner, <br />1978; Anthes et al., 1987; Deardorff, 1972; Zhang and <br />Anthes, 1982; Anthes, 1977). <br /> <br />2. MODEL DESCRIPTION <br /> <br />The model of interest was originally <br />developed by J. Owen Rhea in the 1970's (Rhea, <br />1977). Unlike complex orographic cloud models that <br />attempt to simulate complex cloud processes and <br />consequently require considerable computer resources, <br />Rhea's model attempts to simulate only the most <br />important physical processes that account for much of <br />mountain winter precipitation. <br /> <br />Advantages of such a simple model include ease of <br />performing many iterative runs on relatively <br />inexpensive microcomputers or work stations and <br />operational applicability for hydrometeorological <br />purposes. Additionally, simple orographic <br />precipitation models generally require only routinely <br />collected atmospheric sounding data as input. <br /> <br />The Rhea model is two-dimensional, steady- <br />state, and multi-layer. It accounts for moisture flow <br />from any direction and terrain effects such as rate of <br />rise and "shadowing" by upstream barriers. <br /> <br />The model requires a topographic grid unique <br />to each wind direction. Thus, 36 separate grid arrays <br />of topography are employed, one for each 10" intelVal <br />of the compass, at a selected grid spacing that in the <br />current study was set at 10 kIn. The wind direction at <br />the 850- or 700-mb level at the center of the <br />geographical area of interest is employed to select the <br />particular grid array to be used for model <br />computations. <br /> <br />The model keeps track of condensate <br />formation or evaporation as air layers experience <br />vertical displacements in interaction with the <br />underlying topography. As the model is multi-layer, <br />precipitation falling into a subsaturated layer will <br />partially or totally evaporate. Precipitation developed <br />at higher layers reaches the ground if it is not fully <br />consumed by evaporation. <br /> <br />Simple formulations are included in the model <br />to account for blocking at bw layers and streamline <br />vertical displacement. Enhanced streamline <br />displacement over the highest terrain is used to <br />simulate effects of convection, bUI the model cannot <br />simulate convective cloud processes in any rigorous <br />way. When atmospheric sounding data are available <br />for three or more locations, the model can estimate <br />divergence and include some compensation for large- <br />scale vertical motion. <br /> <br />The model employs a spatially constant <br />precipitation efficiency. The relationship, E = - kTo , <br />where E is the efficiency, k is a positive constant, and <br />To is the temperature in degrees Celsius of the highest <br />layer with relative humidity equal to or greater than <br />65 percent, was found to give satisfactory results <br />provided E was not allowed to exceed 25 percent. <br />
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