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30                                     2  Feedback Control Theory Continued

                        Im                                 Im
                              1 + GH Plane                        GH Plane


                                                         –1
                            0  1      Re                      0         Re
                                         1 + G(jω) H(jω)

                            1 + G(jω) H(jω)                      G(jω) H(jω)



            Fig. 2.8   Plot of 1 + G( iω)H( iω) and G( iω)H 1



              If the mapping theorem is applied to the special case with F( s) = 1 + G( s)H( s),
            then we can make the following statement. Let the closed contour in the s plane cov-
            ering the complete right half of the s plane, then the number of half side of s plane
            zeros of the mentioned function is equal to the number of poles of the mentioned
            function in the right half plane plus the number of clockwise direction of encircle-
            ment of the origin of the closed loop function plane by corresponding closed curve
            in latter plane. Because of this assumed conditions then,

                                 lim (1 Gs+  ( )·H( )) : Constants  =
                               s→ infinity
            The function (1 + G( s)H( s)) remains constant as s traverses the semicircle of infinite
            radius. Because of this, whether the locus of the above function encircle the origin
            of the function plane can be determined by considering only a part of the closed
            contour in the s plane, that is, the imaginary axes. Encirclement of the origin, if
            there are any, occur only while a representative point moves from iω to –iω along
            the imaginary axis, provided that no zeros or poles lie on the imaginary axis.
              Note that the portion of 1 + G( s)H( s) contour from ω = −∞ to ω = ∞ is simply
            1 + G( iω)H( iω). Since the 1 + G( iω)H( iω) is a vector sum of unit vector and the
            vector G( iω)H( iω), 1 + G( iω)H( iω) is identical to the vector drawn from the − 1 + 0i
            point to the terminal point of the vector G( iω)H( iω), as shown in Fig. 2.8. Usually j
            or i is used as complex operator. In Fig. 2.8 j is used as complex operator.
              Encirclement of the origin by the graph of 1 + G( iω)H( iω) is identical to en-
            circlement of the − 1 + i0 point by just the G( iω)H( iω) locus. Thus, stability of a
            closed loop system can be investigated by examining encirclements of the − 1 + 0i
            point by the locus of G( iω)H( iω).
              The number of clockwise encirclement of the − 1 point by the locus can be found
            by drawing a vector from the − 1 point to the GH locus starting from ω = −∞, going
            through ∞ = ∞ and by counting the number of clockwise rotation of the vector. Note
            that the locus of the function when ω goes from infinity to 0 is the mirror image of
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