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Base Station Antennas for Mobile Radio Systems        59

                    At the end of this procedure the currents in each element are given
                  by the vector sum of the currents associated with each excitation that
                  we have applied. To allow for inaccuracy in the practical achievement
                  of the desired current, a margin should be left between the calculated
                  values of nulls and sidelobes and those specified—a margin of 3 dB
                  should generally be adequate. After a suitable array excitation has been
                  produced, it may be modified to suit various practical constraints. It is
                  often convenient to feed adjacent elements with currents of the same
                  amplitude, so for every element pair the mean of the calculated currents
                  can be applied to both. After checking the computed pattern following
                  any adjustments, the required electrical tilt can be arranged by applying
                  a linear phase shift across the array.
                    To provide a fixed electrical beamtilt as a function of frequency, we
                  must delay the currents in lower elements by a fixed time rather than
                  a fixed phase, as our objective is to tilt the phase-front of the radiated
                  signal away from the normal to the array; the phase angle associated
                  with this delay is directly proportional to frequency. This characteristic
                  is provided by different lengths of transmission line rather than by
                  fixed phase shifters. If we compute the cable length differences required
                  at one frequency (typically we do this at midband), the electrical beam-
                  tilt will, in principle, remain constant over the whole band. Errors in
                  the element currents can be regarded as random in phase and with a
                  circular error probable (CEP)—the median length of the error vector
                  of, say, 0.5 dB; the CEP can be increased and a Monte Carlo analysis
                  rerun until a significant number of specification infringements occur.
                  This exercise will indicate the precision that must be achieved in the
                  practical control of the element currents. As an example of what can be
                  achieved, Figure 2.11 shows the superimposed measured elevation pat-
                  terns of a batch of ten 12-element antennas. The degree of consistency
                  of the result is very good above −25 dB.
                    A wide variety of computer-based tools is used for network coverage
                  planning, and unfortunately many of these have adopted inconsistent
                  conventions regarding the format of the input radiation pattern data.
                  Most antenna manufacturers provide radiation pattern data files on
                  their websites and make them freely available in a selection of the more
                  common commercial program formats.

                  2.3.3.3  Input Impedance  The usual specification for the VSWR at the
                  input of a base station antenna is 1.4:1 or 1.5:1. As well as regarding the
                  antenna as a single unit with an input VSWR specification, we need to
                  consider it as a complex assembly of radiating elements, power dividers,
                  and interconnecting transmission lines, and must consider the control
                  of impedance matching at each stage between the radiating elements
                  and the array input. When designing the intermediate components,
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