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100     Chapter Three

                  calculation are varied within a preset range and the element spacing
                  is assumed to be equal to 0.8l o . After the boundaries for the current
                  amplitudes and phases are determined, we need to find the boundaries
                  for the element spacings. By considering the physical sizes of the ele-
                  ments and neglecting the mutual coupling effect between the elements,
                  we assume that the lower and upper boundaries for the element spacing
                  are 0.75l o  and 0.85l o , respectively. Next we need to define the objective
                  functions in the genetic algorithm.
                    Objective Functions  There are several criteria for the radiation pattern
                  to be synthesized. The main lobe has to be synthesized with the absolute
                  maximum value along a specified direction. Also, the power levels of the
                                                                2
                  nulls have to be specified to form a nearly Cosec q pattern. Moreover,
                  the peak gain of the main beam has to be maximized. Other than the
                  radiation pattern, a requirement is also placed on the input return loss
                  of each array element. The objective functions of the genetic algorithm
                  are listed here:
                  ■  Minimum gain > 15 dBi (from 1.71 to 2.17 GHz)
                  ■  Upper sidelobes < −25 dB (from 1.71 to 2.17 GHz)
                  ■  S  < −10 dB, where ii = 11, 22…88 (from 1.71 to 2.17 GHz)
                      ii
                  ■  Peak angle of main lobe = 0° (from 1.71 to 2.17 GHz)
                          2
                  ■  Cosec q pattern (from 1.71 to 2.17 GHz)
                    1.  Lower first null and lower first lobe ∼ −10 dB
                    2.  Lower second null and lower second lobe ∼ −15 dB
                    3.  Lower third null and lower third lobe ∼ −20 dB
                    4.  Lower fourth null and lower fourth lobe ∼ −25 dB
                  ■  The ripples between a null and the nearest lobe are limited to 1 dB
                    difference

                    Practically realizing a cosecant radiation pattern is a difficult task.
                  By using GA, eight objective functions are set to synthesize the cosecant
                  patterns for the eight-element array case. The power levels of the lower
                  first null, lower first lobe, lower second null, lower second lobe, lower
                  third null, lower third lobe, lower fourth null, and lower fourth lobe are
                  included and located in specified angles to form the cosecant pattern.
                    Boundaries of the Variables  Different geometric parameters of the array
                  elements,  including  the  heights  of  the  patches  (h p ),  heights  of  the
                  L-probes (h lp ), lengths of the L-probes (L p ), element spacings of the patches
                  (E 1 , E 2,  E 3,  E 4,  E 5,  E 6,  E 7 ), relative excitation phases of the L-probes (a° n ),
                  and relative excitation amplitudes of the L-probes (|a n |) are adjusted
                  in the optimization process, where n = 1, 2, …, 8. Impedance matching
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