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Biosystems Analysis and Optimization      53


                    40
                 Magnitude (dB)  –20
                    20
                     0



                   –40
                     10 –2       10 –1        10 0        10 1        10 2
                   100
                    50
                 Phase (°)  0


                   –50
                  –100
                     10 –2       10 –1        10 0        10 1        10 2
                                        Frequency (rad/s)
               FIGURE 2.11  Bode plots for constant term K =10 (solid), integral term (dash)
               and derivative term (dot) transfer functions.



               The magnitude is | (Gjω= 20 log ( )  dB; the argument is zero. A gain
                                   )|
                                             K
                                          10
               term has a constant multiplying effect regardless of the frequency, and
               thus merely shifts the overall magnitude plot up or down by a certain
               number of decibels. There is no effect on the phase. The Bode plot of a
               constant term transfer function is illustrated in Fig. 2.11.
               Integral Term (Pole at the Origin)

                                          ω
                                Gs() =  1 ; Gj ) =  1  = −  j       (2.60)
                                        (
                                     s        jω    ω
               The magnitude can then be calculated as

                                   1
                                                      ω
                          |(Gjω )|=  or |(Gjω )|= −20 log ( ) dB    (2.61)
                                  ω                 10
               This means that the magnitude decreases by 20 dB for a tenfold
               increase in frequency. With the frequency ω plotted on a logarithmic
               scale, the magnitude is represented by a straight line of slope –20 dB
               per decade of frequency, which is passing through 0 dB for ω = 1 rad/s.
                   The phase shift for this integral term is

                                                   ω⎤
                               =
                             ω
                                       ω
                                     (
                           (
                          Gj ) arg[ Gj )] = − arctan ⎡ ⎢ ⎥  =−90 °  (2.62)
                                                  ⎣ ⎦
                                                   0
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