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A New  Do11ain  and  More  Process  Models   81

                Question 4-1  Why is the maximum phase lag of the first-order model 90°?

                                  1
                AniWM'  As m, in 8 =  -tan- (0r1 increases without bound to oo, the arctangent
                              1
                function yields  tan- (oo) =  1C /2 or 90°.
              4-1-3  A Uttle Mathematical Support In the Laplace
                     Transform Domain
              From  Chap.  3  and  App.  F,  the  transfer  function  for  the  process
              described by Eq. (4-1) can be obtained directly from Eq. (3-33) by set-
              ting g = 1.0, resulting in

                                 -    1   -    -
                                 Y=--U=GU
                                    -rs+1     P
                                                                  (4-6)
                                      1
                                G  =--
                                 P   t'S +  1
                 Now, another trick! Let s =  j2.1Cf and find the magnitude and the
              phase of the result
                                       1
                          G ('2nf)-
                           pi     --rj2.nf+1
                                  =    1     -r  j2.n f +  1
                                   1' j2.1r f + 1 . -1' j2.1r f + 1
                                  - -1'  j2.1r f +  1
                                         2
                                  - (r2n  f) +  1
                                       1       .   1'2.1r f
                                                     2
                                         2
                                  - (-r2n /) + 1  I (-r2.n /) +  1
                Here, the numerator and denominator of the complex transfer
             function  were  multiplied  by  the  conjugate  of  the  denominator
              -1' j2.n f +  1. This got rid of imaginary components in the denomina-
             tor and allowed us to separate GP into its real and imaginary parts.
                The transfer function is now a complex quantity with a magni-
             tude and a phase, as in




                As shown in App. B, the magnitude of a complex quantity is the
             square root of the real and imaginary parts


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