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56      Chapter Two

                     Materials used successfully have included glass-reinforced plastic
                     (grp/fiberglass),  polystyrene, ABS, ASA,  and  UPVC.  For  outdoor
                     installation,  the  material  must  be  stabilized  against  ultraviolet
                     deterioration. In the case of grp, the resin used must be chosen with
                     care. A typical resin absorbs a sufficient amount of water to change
                     its permittivity between a dried-out condition under prolonged hot
                     sunshine and equilibrium water content in wet weather. In an experi-
                     ment by the author, a pultruded polyester resin grp radome 1.2-m
                     long released a wineglass-full of water (125 g) after being dried out
                     following a 24-hour period of exposure to water on its external sur-
                     faces. The result of water absorption was a substantial increase in
                     the input VSWR of the antenna.
                     There are two contributions to the loss caused by a radome. Loss
                     caused by wave propagation through the thickness of the radome is
                     inevitable, but close placement of the radome to the radiating ele-
                     ments results in further loss caused by stored-energy fields, local to
                     the element, intersecting the radome.
                  k.  The net gain is equal to the directivity of the array (f) minus the sum
                     of all losses (g + h + i + j).

                  2.3.3.1  Elevation Pattern Shaping  Because the user specification relates
                  only to the amplitude and not the phase of the signal radiated at dif-
                  ferent elevation angles, there is no unique set of complex currents that
                  will deliver the specified performance. The antenna designer can choose
                  to constrain a number of variables in order to arrive at a solution that
                  meets the requirements of particular construction methods. A general
                  solution will require both the amplitudes and phases of the radiating
                  currents to be different for each element in the array. Among others,
                  there are classes of solution for which the element currents are equal
                  in magnitude and vary only in phase, solutions in which pairs of adja-
                  cent elements have equal complex currents, and solutions in which the
                  required power dividers have a limited number of simple ratios, suitable
                  for construction from coaxial cables.

                  3.3.3.2   Mutual Impedance  A current flowing in one element of an array
                  induces currents in other elements, particularly in the adjacent ele-
                  ments. The feed impedance of each element is a function of the current
                  that it carries itself and also of the currents in its neighbors. To take a
                  typical example of the third element in a long array:


                                   I       I           I      I
                              Z =  I 1 3  Z +  I 2 3  Z +  Z +  I 4 3  Z +  I 5 3  Z + ...
                                                   33
                                                           43
                                                                  53
                                3
                                       13
                                              23
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