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0066_frame_C27  Page 6  Wednesday, January 9, 2002  7:10 PM









                       difference between the actual magnitude curve and the asymptotic approximation is a function of
                       damping ratio. The resonant frequency  ω r  is defined as the frequency where the peak value of the
                       frequency response M r  occurs. When the damping ratio approaches zero, ω r  approaches ω n . The resonant
                       frequency can be determined by taking the derivative of the magnitude with respect to the frequency,
                       and setting it equal to zero. The resonant frequency and the peak value of the magnitude are represented by

                                                  w r =  w n 12V ,  ς <  0.707                  (27.9a)
                                                               2
                                                           –
                       and

                                                           1
                                                   M r =  -----------------------,  V <  0.707  (27.9b)
                                                       2V 1 V  2
                                                            –
                       Example 2
                       Let us consider the transfer function
                                                             10 s/5 + 1)
                                                               (
                                               Gs() =  ----------------------------------------------------------------------
                                                             (
                                                            [
                                                       (
                                                      ss + 1) s/10) + ( s/10) + 1]
                                                                  2
                       We first list the basic factors of G(s) in Table 27.1 in the order of increasing corner or natural frequencies.
                         The complete asymptotic magnitude curve for G(jω) is produced by adding together the asymptotic
                       logarithmic magnitudes of each factor, as shown by the solid line in Fig. 27.6. Since the dc gain of each
                       factor is 1, these factors have no effect on the asymptotic magnitude until the frequency approaches their
                       corner or natural frequencies. Thus, the asymptotic magnitude can be quickly obtained by plotting each
                       asymptote in order as frequency increases. The asymptotic curve intersects 20 dB at ω  = 1 with the slope
                       −20 dB/decade due to the pole at the origin and the constant gain K = 10. At ω  = 1 the slope further
                       decreases to −40 dB/decade due to the pole at ω  = 1. Then at ω  = 5 the slope increases to −20 dB/decade


                                     TABLE 27.1  The Basic Factors of G(jω)
                                     Type of Factors  Constant Gain  Pole  Pole  Zero  Complex Poles
                                     Corner frequency  K = 10   0    1    5       10
                                     Order             0       −1   −1   +1       −2



                                              40
                                                       −20 dB/dec   Exact curve
                                              20
                                            Magnitude (dB)  −20 0  −40 dB/dec   −20 dB/dec   −60 dB/dec
                                                                      Exact curve
                                                           Asymptotic curve
                                             −40
                                             −60
                                             −80
                                             −90
                                                              Exact curve
                                                 −45 deg/dec
                                             −135     0 deg/dec
                                            Phase (deg)  −180  −90 deg/dec   −45 deg/dec
                                             −225            Asymptotic curve   −90 deg/dec
                                             −270
                                              0.1         1          10         100
                                                            Frequency (rad/s)
                       FIGURE 27.6  The Bode plot of the transfer function in Exmple 2.


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