Page 151 - Satellite Communications, Fourth Edition
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Polarization  131

                                Maximum values quoted by Miya (1981) for Faraday rotation are 9°
                              at 4 GHz and 4° at 6 GHz. In order to counter the depolarizing effects
                              of Faraday rotation, circular polarization may be used. With circular
                              polarization, a Faraday shift simply adds to the overall rotation and does
                              not affect the copolar or cross-polar components of electric field.
                              Alternatively, if linear polarization is to be used, polarization tracking
                              equipment may be installed at the antenna.


                              5.6 Rain Depolarization

                              The ideal shape of a raindrop is spherical, since this minimizes the
                              energy (the surface tension) required to hold the raindrop together. The
                              shape of small raindrops is close to spherical, but larger drops are better
                              modeled as oblate spheroids with some flattening underneath, as a
                              result of the air resistance. These are sketched in Fig. 5.12a and b. For
                              vertically falling rain, the axis of symmetry of the raindrops will be
                              parallel to the local vertical as shown in Fig. 5.12b, but more realisti-
                              cally, aerodynamic forces will cause some canting, or tilting, of the drops.
                              Thus there will be a certain randomness in the angle of tilt as sketched
                              in Fig. 5.12c.
                                As shown earlier, a linearly polarized wave can be resolved into two com-
                              ponent waves, one vertically polarized and the other horizontally polar-
                              ized. Consider a wave with its electric vector at some angle t relative to
                              the major axis of a raindrop, which for clarity is shown horizontal in
                              Fig. 5.13. The vertical component of the electric field lies parallel to the
                              minor axis of the raindrop and therefore encounters less water than the hor-
                              izontal component. There will be a difference therefore in the attenuation
                              and phase shift experienced by each of the electric field components. These
                              differences are termed as the differential attenuation and differential phase
                              shift, and they result in depolarization of the wave. For the situation shown
                              in Fig. 5.13, the angle of polarization of the wave emerging from the rain
                              is altered relative to that of the wave entering the rain. Experience has













                                   (a)                    (b)                       (c)
                              Figure 5.12 Raindrops: (a) small spherical, (b) flattening resulting from air resistance,
                              and (c) angle of tilt randomized through aerodynamic force.
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