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116                                 Modern Control of DC-Based Power Systems


             After the compensation a linear system is present, where the classical
          pole placement technique can be performed so that the natural frequency
          and damping coefficient are shifted to the desired values. Additionally, a
          PI controller is added in parallel, which drives the system output to the
          reference value.
             It is possible to make an analogy to terrestrial power systems where
          the fast stabilizing action of the LSF corresponds to the primary control
          action, while the slower dynamics where the PI control bring the system
          to the reference value corresponds to a secondary control action in terres-
          trial power systems.
             In the following, it is shown how to achieve LSF using the general
          approach of [6]. Furthermore, it is explained how the control law can be
          developed from conditions on the natural frequency and damping ratio as
          it was done in [10]. Additionally, the derivation of the control law incor-
          porates the Lie derivative.
             As explained in Section 5.2, the cable parameters can be neglected
          and the CPL capacitances and output filter capacitances can be replaced
          by an equivalent component: C eq 5 C CPL 1 C f 1  1 C f 2 1 C f 3
             The system can be derived from the model in Fig. 5.2 as follows:

                               1                 V       P eq
                          _ V 5   I 1 1 I 2 1 I 3 Þ 2  2
                                 ð
                              C eq             R L C eq  C eq V
                                                                      (5.14)
                                       V     d k UE k
                         _
                               R fk
                         I k 52    I k 2  1       fork 5 1; 2; 3
                                L fk   L fk   L fk
             To shorten the calculations a time constant T f 5  L fk  is defined. This is
                                                         R fk
          only valid if the ratios are equal for all filters. Besides, the equations are
          simplified by summing up the inductances   1  5  1  1  1  1  1  and
                                                     L eq  L f 1  L f 2  L f 3
          currents i 5 I 1 1 I 2 1 I 3 .
                             I      V       P eq
                        _ V 5   2        2
                             C eq  R L C eq  C eq V
                                                                      (5.15)
                               1     V     d 1 E 1  d 2 E 2  d 3 E 3
                        _ I k 52  I 2   1       1      1
                               T f   L eq  L f 1   L f 2  L f 3

             Still, the system description (5.15) is not ideal for the LSF design as it
          is described in [6]. Therefore, the following state-space representation
          will be used to show the transformation of the system:

                                   _ x 5 AðxÞ 1 BxðÞUu
                                                                      (5.16)
                                  y 5 c xðÞ
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