Laserfiche WebLink
<br />~ <br /> <br />During the 1968-69 operational season at the Park Range location, a Nike <br />Ajax radar at Mt. Harris and a GPG-1 radar at Lodwick were used to ob- <br />tain quantitative profile estimates of precipitation over the target area. <br />This was accomplished using a variation of the well known radar range <br />equation which is given by Battan (1960) as: <br /> <br />I; <br /> <br />P = <br />r <br /> <br />P + G2 >.. 2 <br />t <br />(41T)3 R: <br /> <br />(1) <br /> <br />where <br /> <br />P <br />r <br /> <br />received power in Watts. <br /> <br />Pt = peak transmitted power in Watts. <br /> <br />G = Antenna Gain <br /> <br />>.. = Wave length of radar in cm. <br /> <br />a = Target backscatter cross section in cm2 <br /> <br />Rt = Range to the observed target in cm. <br /> <br />The variation used for weather scatterers is accomplished according to <br />Atlas and Mossop (1960) by substituting for <br /> <br />'~ <br /> <br />0' = NV <br /> <br />(2) <br /> <br />~ <br /> <br />Here V is the pulse volume given by Handman and Davis (1964) as: <br /> <br />V::: <br /> <br />2 <br />1T Rt e 0 h <br />8 <br /> <br />e = horizontal beam width in radians <br /> <br />o vertical beam width in radians <br /> <br />h = the pulse length in space <br /> <br />-1 <br />The quantity N is the reflectivity of the particles in cm and if expressed <br />in the usual form after Atlas and Mossop (1960) involving the reflectivity <br />factor Z is: <br /> <br />N = <br /> <br />10-121T5K2 Z <br />>..2 <br /> <br />(3) <br /> <br />: <br /> <br />20 <br />