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Base Station Antennas for Mobile Radio Systems        53

                  downward, the upper grating lobe will grow in amplitude and the loss
                  of directivity caused by overspacing will increase. We must, therefore,
                  choose the element spacing after computing the directivity/frequency
                  relationship with the maximum required electrical tilt applied. The rate
                  at which the grating lobes grow as the spacing exceeds 1l depends on
                  the elevation pattern of the individual elements—those with significant
                  radiation close to the array axis must be spaced closer than elements
                  with low radiation in this direction.
                    To optimize both the technical and the economic parameters of array
                  design, establishing a gain budget is helpful (Table 2.2). Begin with an
                  estimate of the number of elements needed (n) and repeat the process
                  for a different number if the calculated net gain is unsatisfactory.


                  TABLE 2.2    Gain Budget
                    Reference
                    (see below)                  Parameter                    dB
                       a       Directivity of a uniform array of n omnidirectional elements
                               at the chosen spacing
                       b       Reduction in directivity at band edges
                       c       Beam shaping loss
                       d       Allowance for imperfect current distribution
                       e       Max/mean power ratio of the azimuth pattern
                       f       Directivity of the array
                       g       Loss in radiating elements
                       h       Attenuation in feed network
                       i       Attenuation of cable from connector to primary power
                               divider
                       j       Radome loss
                       k       Net gain


                  a.  This value is obtained by integration of the elevation pattern of a
                     collinear array of the chosen radiating elements. For a vertically
                     polarized array an approximation may be made by using the pat-
                     terns for an array of short vertical dipoles, but for slant-polarized
                     arrays this approximation may lead to underestimation of the grat-
                     ing lobes and a consequent overestimation of the directivity of the
                     real array. The elevation pattern maximum of individual tiers must
                     lie in the horizontal plane. Although the beamtilt of the array will
                     be determined by the array factor, if the individual tiers fire slightly
                     upward, the maximum total directivity will be reduced, especially
                     for arrays with a large electrical downtilt. A slight downward tilt is
                     more acceptable because the element pattern and the array factor
                     are likely to be tilted in the same direction.
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