Page 284 - Maxwell House
P. 284

264                                                       ANTENNA BASICS

        are interrelated  through the two  electric  lengths:   = ( + 1)   and  = ( + 1) .
                                                                      
        Since they are independent, the designer can realize (depending on system specification) a wide
        diversity of patterns with different shapes in the elevation and azimuth plane. For example, the
        pattern can be broad in elevation plane and much narrower in azimuth (typical for air traffic
        control radars) or vice versa (typical for broadcast and some communication systems). Figure
        5.6.4a depicts this kind of patterns. Note that the level of the highest sidelobes is around -13dB
        in both planes which is just slightly lower than in linear array with the same uniform excitation.

        The sidelobe level (SLL) and the pattern with specially shaped envelope can be controlled by
        an appropriate inter-element, magnitude and sometimes phase tapering or weighting in the same
        way as in linear arrays. In particular, the excitation reduction from the maxima in the array
        center to its edges actually reduces SLL but widens the main beam as Figure 5.6.4b depicts.
        Chebyshev’s or any other synthesis technique can be applied independently for each pattern
        cut.  Figure  5.6.4b  demonstrates the one plane  sinus-tapered  when | | = 1, | | =
                                                                            
            
        sin � � ,  = 0,1, … , . As expected, SLL peak drops to -23.2dB in the azimuth cut  = 0 and
            
        does not change, i.e. around -13dB, in the cross section  = 90°.
        Figure 5.6.5a shows the 2D sector pattern with a flat top and sinus-tapering that is similar to
        the depicted in Figure 5.4.4. This planar array comprises 31x31 radiators.
        The beam steering technique is exactly the same as in a linear array and can be provided by
        variable phase shifters, TTD  units,  and frequency change. Note that the number of these
        managing the beam angular position elements increases proportionally to 2∙(M+1)∙(N+1) and
        reaches many thousands in a large array providing the transmitting and receiving functions.
        Figure 5.6.5b demonstrates the grating lobe appearance when the main beam is steered too far
        from the zenith by a plane array of 16x16 radiators. The picture-in-picture is the image of a
        142-meter-high (466 feet) skyscraper in Barcelona in Spain designed by French architect Jean
        Nouve. The resemblance is a curious but not unusual coincidence exposing the hidden beauty
        of array design.
        Figure 5.6.5a shows the 2D sector pattern with a flat top and sinus-tapering that is similar to
        the depicted in Figure 5.4.4. This planar array comprises 31x31 equally spaced radiators.


                                                       Grating  Steered at 60
                                                        Lobe    Main Beam









                                         a)                                  b)

                 Figure 5.6.5 Planar array pattern: a) Sector-shaped, b) With grating lobe
   279   280   281   282   283   284   285   286   287   288   289