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WMOD00296 (2)
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Last modified
7/28/2009 2:34:16 PM
Creation date
4/11/2008 3:45:00 PM
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Template:
Weather Modification
Contract/Permit #
14-06-D-5640
Title
Park Range Atmospheric Water Resources Program Final Report
Date
9/30/1969
Weather Modification - Doc Type
Report
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<br />~ <br /> <br />SECTION 3. 0 <br />SPECIAL SU PPORT STUDIES <br /> <br />~ <br /> <br />3. I Numerical Models <br /> <br />The advantages of applying numerical studies to experimental cloud seeding <br />projects come from the ability to separate and study the various physical <br />processes, and to isolate their effects on precipitation. Evaluation techniques <br />are enhanced by the predictions of a realistic model that can be compared to <br />observed values. Various modification techniques can be simulated and the <br />model used as a tool to optimize the effect of modification procedures. The <br />basic model used on this project has been d~scribed in previous reports, but <br />a brief description of the model, as well as present and projected improve- <br />ments, is included here. <br /> <br />3. 1. 1 Two Dimensional Mountain Airflow <br /> <br />In the flow section of the model the motion is considered to be in an (x, z) <br />plane with the x-axis along the wind and z -axis in the vertical. The total <br />flow in this plane can be separated, using perturbation techniques, into a <br />steady basic current and a small perturbation current. Adiabatic steady <br />state frictionless motion is assumed. After solving the equations for the <br />differential form of the perturbation velocity and neglecting the smaller <br />terms <br /> <br />.., <br />v <br /> <br />,,2 w <br />" z2 <br /> <br />2 <br />+ (f(z) - k ) w == 0 <br /> <br />(7) <br /> <br />where w is the amplitude factor of the vertIcal velocity (sinusoidal with wave <br />number k) and <br /> <br />f (z) <br /> <br />=~ <br />2 <br />u <br /> <br />+ <br /> <br />( :2z~ ) <br /> <br />u <br /> <br />(8) <br /> <br />This equation has been used for most of the past work on mesoscale flow over <br />mountains (Queney 1947, Scorer 1949, Wurtele 1953, Palm 1958, Sawyer <br />1960). Methods of solving it differ in detail but, in general, some simple <br />distribution of f (z) has been chosen and Fourier's theorem used. <br /> <br />If the sinusoidal lower boundary condition is of the form <br /> <br />1::0 = f (k) cos kx = ha exp (-ak) cos kx <br /> <br />(9) <br /> <br />the equation may be integrated over all wave numbers to give an ideal moun- <br /> <br />40 <br />
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