Page 527 - Mechanical Engineers' Handbook (Volume 2)
P. 527

518   Control System Performance Modification

                             If G(s)H(s) has a single parameter K as a variable, then by rewriting as
                                                      1   KG(s)H(s)   0                        (8)

                          a standard procedure for obtaining the closed-loop poles corresponding to any K is the Evans
                          root-locus method.


           5.1 Angle and Magnitude Conditions
                          The CLCE [Eq. (8)] can be written as
                                                   KG(s)H(s)   1   e j(2  /   )                (9)

                                         satisfying the condition
                          Thus, any point s 0
                                                   / KG(s )H(s )   (2l   1)                   (10)
                                                        0
                                                            0
                          satisfies Eq. (8). If K   0, then Eq. (10) reduces to
                                                    / G(s )H(s )   (2l   1)                   (11)
                                                           0
                                                       0
                          and is commonly called the angle condition. All points s in the complex plane satisfying
                                                                       0
                          this angle condition satisfy the closed-loop characteristic equation and hence are said to lie
                          on the root locus. If s is a point on the root loci, then the corresponding value of K may
                                           0
                          be computed by noting that
                                                       K  G(s )  H(s )    1                   (12)
                                                                0
                                                           0
                          which is called the amplitude condition.
                             By studying the angle condition in detail of the CLCE,
                                                                   	 m  (s   z )
                                              / 1   KG(s)H(s)   1   K  i 1  i
                                                                   	 j 1 (s   p )
                                                                     n
                                                                            j
                          a set of rules can be developed for constructing the root locus easily. These rules are given
                          next without proof. 2
                          Rule 1. The system root loci have n branches originating at the n open-loop poles  p , j
                                                                                             j
                             1,..., n, with the value K   0.
                          Rule 2. Out of the n branches m number of branches will terminate on m finite zeros  z , i
                                                                                                i
                               1, 2,..., m, of the open-loop transfer function at K   .
                          Rule 3. The remaining n   m branches will go to   along asymptotes as K →  . The
                             asymptotes are straight lines meeting at a point on the real line called the hub with
                             specific orientation as given in rule 4.
                          Rule 4. a. The asymptotes meet at the hub
                                                          n  poles     m  zeros
                                                    
    j 1        i 1
                                                               n   m
                                                          n  ( p )     m  ( z )
                                                         j 1  j     i 1  i
                                                              n   m
   522   523   524   525   526   527   528   529   530   531   532