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Control Approaches for Parallel Source Converter Systems     149


              5.4.1.3 Augmented Kalman Filter
              Typically ISPSs can be divided in local subsystems with local states x i
              which are dynamically coupled such as in Fig. 5.7. In the context of a
              decentralized control architecture which is able to accommodate sudden
              changes in topology and operates without the need of additional measure-
              ments, each subsystem assumes to lump the nonlocal part into an equiva-
              lent virtual source. Additionally, this source is considered to be a
              disturbance with unknown dynamics as it is illustrated in Fig. 5.23.
                 It is considered now that the ISPS can be represented by a LTI system
              like (5.97). This allows expressing any subsystem as [32]:
                                                    m
                                                   X
                                 _ x i 5 A i x i 1 B i u i 1  F i x j   (5.102)
                                                  j5k;j6¼1
                                             m
                                            X
                                 _ y 5 C i x i 1                        (5.103)
                                  i              G i x j 1 H i v i
                                           j5k;j6¼1
                 Where the local state vectors are x i and u i and y represent the local
                                                             i
              measurements which are degraded by the noise v i . The remote j-th sub-
              system is represented by its state x j . The interaction between subsystems
                                         m         m
                                        P         P
              are represented by the terms  F i x j ,  G i x j .
                                       j5k;j6¼1  j5k;j6¼1
                 Incorporating now the concept of a virtual disturbance source, defined
              in [32], into the Eqs. (5.117) and (5.118) and denoting it with x di permits
              to define the following system model:

                                    _ x i 5 A i x i 1 B i u i 1 D i x di  (5.104)
                                                                        (5.105)
                                    _ y 5 C i x i 1 E i x di 1 H i v i
                                    i
                 Where the terms related to x di have now substituted the interconnec-
              tion terms, and therefore the local subsystem dynamics depend only on
              these states and the dynamics of the virtual disturbance. As the virtual



                                R f  L f  I L          PCC

                                                            I   I
                          d·E           C f  V   R L  I d    1   k


              Figure 5.23 Decentralized model including the virtual disturbance.
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