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254                                                       ANTENNA BASICS


                                                  ⁄
                                        ⁄
                                              ⁄
        90° to 30°. If so,    = 30° and   < 1 �√3 2 + 1� = 0.536. Note that moderate rise
        in the equivalent or real phase velocity above the light speed, i.e. / < 1, allows us to slightly
                                                               
        push elements apart.
        Note that the array system comprised of separate receive and transmit array could improve
        situation with grating lobes if a beam of receive array has nulls in the direction of transmit array
        grating lobes. Consequently, the “two way” pattern of such system would be free of grating
        lobes.
        5.5.4   True Time Delay (TTD) Steering

        Simple inspection of equation (5.91) reveals a distressing phenomenon of the beam squint. It
        means that the main beam points in exactly the right direction  =    only if  =   and
                                                                   0
        diverges from this angle as frequency deviates. The plots in Figure 5.5.4a clearly illustrate this
        effect causing system signal distortion as a consequence of undesired amplitude and phase
        modulation (see (5.91)). To explain the nature of this effect recall that the phase difference  =
        −cos = −(2/)cos between fields emitted by the adjacent radiators is proportional
        to frequency while the inter-element phase shift  provided by the phase shifters is fixed and
        practically  independent  on  frequency.  As  a  result,  the  difference   −  = −cos ∓
         cos    and thus the  main beam  maxima at   =     are  frequency dependent.
         0
        Theoretically, the solution is straightforward and follows from the latter expression. We must
        develop a phase shifter providing the frequency progressive inter-element phasing, i.e.  =
















           Figure 5.5.4 a) Frequency beam squint in the broadband linear array, b) The same array
                                          with TTD

                                                   ) and the linear array becomes squint-free
        ±cos  . Then  −  = −(cos − cos 
                                                     ⁄
        (see Figure  5.5.4b). Note that the  time delay   =   = ±(2/)cos    of signal
        passing such phase shifters is constant, i.e. frequency independent. From here, the term “true-
        time-delay” is derived.
        The question boils down how to do it practically. Let us consider the schematic block diagram
        presented in Figure 5.5.5a that is equivalent to Figure 5.4.9c where the fixed phased shifters are
        replaced with TTD units maintaining the progressive time delay and are integer multiples of .
        Each TTD unit is a section of transmission line defined as any structure that is capable of
        carrying  electromagnetic wave energy  with  little  loss.  It  can be the parallel line, i.e.  two
        conductor line, coaxial cable, stripline, waveguide, optical fiber, and many others. We refer the
        reader to Chapter 6 for details.
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