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Last modified
7/28/2009 2:37:39 PM
Creation date
4/16/2008 11:05:22 AM
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Weather Modification
Title
WMO Training Workshop on Weather Modification for Meteorologists - Lecture Notes
Date
12/1/1979
Weather Modification - Doc Type
Report
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<br />- 37 - <br /> <br />This expiession differs from the preceding one only by the multiplier <br /> <br />1 <br />21 n 2 . <br /> <br />For <br />the <br />the <br /> <br />a single spherical scatterer, whose dimensions are <br />wavelength (f:: 0.1 ). ), the back-scattering cross <br />sphere's diameter Do by the relationship: <br />5 2 6 <br />iT =., I K I Do <br />). <br />= n - iK) ~s the <br /> <br />small in comparison with <br />section is connected with <br /> <br />m 2 _ 1 <br />where K = 2 ' and m ( <br />m + 2 <br /> <br />This relationship is called Rayleigh's law" The constant characterizing the <br /> <br />refraction depends on temperat~re, wavelength and particle composition. For wave- <br /> <br />lengths > 1 cm and for the whole tempereJture range in the atmosphere <br /> <br />I K ,2::::: 0.93 for water and 0.21 for iCEl. <br /> <br /> <br />2.13 For a combination of spherical pa~ticles which are small by comparison <br />with the wavelength the mean power of the received signal is <br /> <br />sphere's combined refractive index. <br /> <br /> p Pt G2e'~h1l"3 II< I 2 D.6 <br /> r - - . L <br /> ~6 4 Sin (2).2T2) i ~ <br /> L <br />where i ~ designates, as above, the summation over a unit volume. <br /> <br />2.14 Thus, for spherical scatterers which are small compared with the <br />wavelength, the mean power of the received signal is determined by the radar's <br />parameters, the distance to them and only two multipliers which depend on the <br />scatterers themselves, <br /> <br />IK I 2 <br /> <br />" D.6 <br />and 'l:' ~ <br /> <br />Because of the importance of the second multiplier in meteorological radar a new <br />value Z is introduced, called the radar reflectivity, and can be determined as <br />follows: . <br /> <br />~ <br />where ~ designates the summation over a unit volume, and N (D) is the number <br />of scatterers in the diameter range D to D + d D in the unit volume. N (D) <br />designates the raindrop size distribution and for snow crystals the drop diameter <br />distribution obtained after melting. (If such a determination is not made for <br />snow, the snow's density within the crystals must be taken into account in the <br />multiplier I K I 2 .) <br /> <br />z = ~ Di 6 = f N ( D ) <br />~ <br /> <br />D 6 d D <br />
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