Page 414 - Maxwell House
P. 414

394                                                                Chapter 8



            dielectric substrate, i.e. it is shorter than in free space. Note that PD = 3 dB (thicker magenta
            solid curve) corresponds to the couplers in which the input power from port1 is divided
            equally between port3 and port4. They belong to a special class of couplers named hybrids.
        8.  It may seem surprising, but this coupler provides the frequency independent phase shift of
            90° between signals coming to port2 and port3. This feature combined with 3 dB power
            division  makes them  the  universal element of coherent power combiners and splitters,
            diplexers, balance amplifiers, phase shifters, mixers, phased array beam-forming networks,
            and many other applications.
        9.  The described theory of couplers is based on the assumption that the even- and odd-mode
            have the same or very closed propagation constant. Generally, it is not quite right because
            both modes are quasi-TEM only. As we have mentioned before, any deviation from TEM
            makes the mode propagation constants frequency dependable. The most troubling is that
                                   ±    ++                              ±   ++ . If so,
            they become not equal, i.e.  ≠   , i.e. possess different wavelengths  ≠ 
            how to meet the requirement that the coupler length should be quarter-wavelength? Which
            of them? That is not the issue for narrow banded couplers but the serious limitation for
            wideband design due to fast deterioration of directivity and isolation. Therefore, we need
            some technique to equalize the even- and odd-mode propagation constant. Typically, it
            requires slowing the odd-mode while  leaving the even-mode propagation constant
            practically unchanged. Figure 8.2.4c and Figure 8.2.4d illustrate two approaches. Both as
            many others are based on the differences in EM field structures of modes. In so-called
            wiggly coupler in Figure 8.2.4c, the odd-mode should follow the saw tooth path and
            thereby slows down (green line) due to the most part of its energy concentrated into and
            nearby the gap. Meanwhile, the energy of even-mode is accumulated in dielectric substrate.
            If so, this mode barely notices the presence of a gap and practically does not slow down
            (red line). The analogous effect occurs in forward (blue line) coupler with shunt periodic
            stubs depicted in  Figure 8.2.4d. According to [1] such coupler has  good performance
            covering from 2 GHz to 4 GHz.


        We shall not pursue this subject here anymore asking the reader to turn to the appropriate
        literature [3, 8] for more information. Note that such kind of directional coupler can be realized
        using almost any type open and closed transmission line including the optical lines.
        8.2.4   WR Hybrids

        As we have mentioned before, hybrids as well as 3-dB couplers, belong to the broad family of
        four-port power dividers/splitters with an equal power split, i.e. 3-dB split, between two ports
        keeping one of the ports isolated. The effect of isolation may be accomplished by means of
        particular geometrical structure (like WR magic-T) or wave interference at the isolated port
        (like ring or branch hybrid).
                                                           4
        Let us start from so-called WR magic-T shown in Figure 8.2.5a . It incorporates two WR tees:
        H-plane tee formed by WR of ports 1, 2, 3 and E-plane tee shaped by WR of ports 2, 3, 4.
        Remind that the term H-plane means that the WR branches are located in the plane containing
        H-field vector while E-field vector belongs to E-plane.





        4  Public Domain Image, source: http://www.slideshare.net/KaziMdRahaman/seminar-on-magic-tee
   409   410   411   412   413   414   415   416   417   418   419