Page 97 - Mechatronics with Experiments
P. 97

CLOSED LOOP CONTROL  83
                                                                           2 1∕2 j tan −1 (w∕z i )
                                                     = (jw∕z + 1) = [1 + (w∕z ) ]  e            (2.73)
                                         (s∕z + 1)|
                                            i    s=jw      i              i
                                                                     2 1∕2
                                                                                         2 1∕2
                                      20 log |jw∕z + 1| = 20 log [1 + (w∕z ) ]  = 20 log [1 + (w∕z ) ]  (2.74)
                                                                    i
                                                                                        i
                                                i
                                                     =≈ 20 log 1 = 0;  for w∕z ≪ 1              (2.75)
                                                                            i
                                                     =≈ 20 log(w∕z );  for w∕z ≫ 1              (2.76)
                                                                            i
                                                                 i
                                                         −1
                                          ∠(jw∕z + 1) =tan (w∕z )                               (2.77)
                                                i
                                                               i
                                  The Bode plots of first-order (real) poles and zeros are also shown in Figure 2.30.
                                4. Second-order (complex conjugate) poles and zeros: Consider a complex conjugate
                                  pole pair, and its frequency response
                                            1                                  1
                                                      | s=jw  =                           (       )
                                        2
                                   (s∕w ) + 2  (s∕w ) + 1                             j tan −1  2  w∕w i
                                       i
                                                 i
                                                                                                2
                                                                                 2 1∕2
                                                                  2
                                                                     2 2
                                                            [(1 − w ∕w ) + (2  w∕w ) ]  e   1−(w 2 ∕w )
                                                                                                i
                                                                     i          i
                                                                                                (2.78)
                                  The magnitude and phase as function of frequency are given by
                                                                         2 2
                                                                                     2 1∕2
                                                                     2
                                               20 log | ⋅ | =−20 log[(1 − w ∕w ) + (2  w∕w ) ]  (2.79)
                                                                         i         i
                                                       ≈ 0;  w∕w ≪ 1                            (2.80)
                                                                 i
                                                       ≈−40 log(w∕w );  w∕w ≫ 1                 (2.81)
                                                                    i       i
                                                                (           )
                                                                   2  (w∕w )
                                                             −1          i
                                                   ∠(⋅) =− tan                                  (2.82)
                                                                       2
                                                                          2
                                                                 (1 − w ∕w )
                                                                          i
                                  Similarly, the Bode plot of a complex conjugate zero and its asymptotic plot can be
                                  found as (Figure 2.30).
                                                                                           (      )
                                                                                       j tan −1  2  w∕w i
                                        2                         2  2 2          2 1∕2     1−(w 2 ∕w )
                                                                                                 2
                                   (s∕w ) + 2  (s∕w ) + 1|  = [(1 − (w ∕w )) + (2  w∕w ) ]  e    i
                                       i         i    s=jw           i           i
                                                                                                (2.83)
                                                                        2 2
                                                                                     2 1∕2
                                                                     2
                                               20 log | ⋅ | = 20 log[(1 − (w ∕w )) + (2  w∕w ) ]  (2.84)
                                                                        i          i
                                                       ≈ 0;  w∕w ≪ 1                            (2.85)
                                                                 i
                                                       ≈ 40 log(w∕w );  w∕w ≫ 1                 (2.86)
                                                                          i
                                                                  i
                                                              (           )
                                                                 2  (w∕w )
                                                                       i
                                                            −1
                                                   ∠(.) =tan                                    (2.87)
                                                                        2
                                                                     2
                                                                1 − (w ∕w )
                                                                        i
                             Nyquist (Polar) Plots of Standard Elements of a Transfer Function
                             Nyquist plots (also called polar plots) are the graphical representation of the frequency
                             response data on a complex plane where the y-axis is the imaginary part, and the x-axis is
                             the real part of the frequency response. The frequency is parameterized along the curve.
                                                        = Re(G(jw)) + jIm(G(jw)) = X(w) + jY(w)  (2.88)
                                         G(jw) = G(s)| s=jw
                             For every point along the imaginary axis of the s-plane, s = jw, there is a point on the
                             curve plotted on the (G(jw))-plane. Nyquist plots of various standard elements are shown
                             in Figure 2.31.
                             Log Magnitude versus Phase Plots of Standard Elements of a Trans-
                             fer Function   Frequency response is conveniently represented by a complex function.
                             Graphical representation of a complex function must convey the real and imaginary part or
                             magnitude and phase information. Another possible way of plotting the frequency response
   92   93   94   95   96   97   98   99   100   101   102