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376                                                                Chapter 7



        The first two expressions are the simple balance of active power taking place in the lossless
        circuit  where 1 is the normalized input  active  power.  From them  we get  | |= | |
                                                                           22
                                                                                 11
        and | | = �1 − | | . The last equity in (7.13) is the consequence of the reactive power
                           2
             21
                         11
        balance where 0 means the absence of the input and output reactive power. It reveals that the
        phase of  transmission coefficient   21  = | |  21   and reflection coefficient   11  =
                                               21
        | |   11 must be mutually dependent parameters
          11
                                      2 21  =  11  +  22 +                  (7.14)
        Therefore, the reciprocal and lossless 2-port network could be described by the single complex
        parameter   or two reals | | and   as soon as it is
                                       11
                               11
                  11
                                                                  2  11
                                              11    �1 − | | 
                                                               11
         Symmetrical, i.e.  22  =   and  = �               �
                             11
                                       �1 − | |    11
                                                 2  11
                                               11
                                                      �1 − | | 
                                                                   2  11
         Asymmetrical, i.e.  22  = −  and  = �  11   11     �        (7.15)
                               11
                                                   2  11
                                          �1 − | |     − 11
                                                11
        Evidently, all discontinuities in Table 7.1 and 7.2 fall into one of these categories.
        7.3.4   Scattering Transfer T-Matrix
        The S-matrix introduced in the previous section is a very convenient way to describe an N-port
        network linking the reflected  wave on one port  with incident  waves in all others.  Such
        description is very  well adapted to measurements and simulations but becomes  slightly
        problematic for the description of the multiple networks connected in a cascade like shown in
        Figure 7.3.3a. The equivalent circuit of a transmission line demonstrated in Figure 6.1.2b is
        exemplary. A common class of filters, phase shifters, matching devices, and a wide range of
        RF components  are realized  by cascading  simple  resonance, switching elements, or other
        discontinuities. To simplify the discussion, the following analysis is limited to the sequence of
        2-port networks. It turns out that in the cascade the output of one network feeds the input of the
        next and so on. If so, we need a matrix that links not the incident and reflected waves somewhere
        around the networks but directly relays the input  ,   and output  ,   waves as
                                                               2
                                                   1
                                                                 2
                                                1
                                       11   12   2
                                     1
                                   � � = �        � �  �                        (7.16)
                                     1   21   22   2












        Figure 7.3.3 T-matrix illustration: a) Cascaded 2-port network, b) Incident (blue) and reflected
                                         (red) waves
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