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Small-Signal Analysis of Cascaded Systems                     53


                                                                 1
                       V out L             Z in L
                 G SL 5       5 G S G L U           5 G S G L U          (2.93)
                        V in S         Z in L 1 Z out S      1 1 T MLG
              where the minor loop gain T MLG is defined as

                                               Z out S
                                       T MLG 5                           (2.94)
                                               Z in L
                 It is called minor loop gain because it can be shown that the output
              impedance of the source subsystem Z out S and input impedance of the
              load subsystem Z in L form a type of negative feedback system as depicted
              in Fig. 2.28.
                 Since G S and G L are stable transfer functions, the minor loop gain
              term is the one responsible for stability. Therefore, a necessary and suffi-
              cient condition for stability of the cascade system can be obtained by
              applying the Nyquist Criterion to T MLG , i.e., the interconnected system
              is stable if and only if the Nyquist contour of T MLG does not encircle the
              ð2 1; j0Þ point. From the control theory of linear systems, two quantities
              called Gain Margin (GM) and Phase Margin (PM) can be defined. These
              quantities quantify “how far” the Nyquist contour of T MLG is from the
              critical ð2 1; j0Þ point, and, therefore, “how far” the system is from being
              unstable. The quantities GM and PM are also related to the dynamic
              response of the system: the higher the damping, the larger GM and PM
              are (and vice versa the lighter the damping, the smaller GM and PM are)
              [22]. Specifying GM and PM provides the engineers a way to design for
              system stability with certain stability margins linked to the desired
              dynamic time domain performance. Based on this concept, what is practi-
              cally needed is to guarantee that the Nyquist diagram of T MLG does not
              encircle the ð2 1; j0Þ point with sufficient stability margins. For this rea-
              son, many practical stability criteria for the cascade system of Fig. 2.28
              were proposed. These stability criteria define various boundaries between
              forbidden and allowable regions for the polar plot of T MLG . The bound-
              aries are defined by a certain GM and PM and are shown in Fig. 2.29.
              The forbidden regions are the ones that include the ð2 1; j0Þ point.
              System stability can be ensured by keeping the contour of T MLG outside
              the forbidden regions. Based on the definition of the forbidden regions,
              design formulations can be specified which relate the desired GM and
              PM to the system parameters. Note that these criteria give only sufficient,
              but not necessary stability conditions.
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