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                                                            Power electronic control in electrical systems 305















                      Fig. 8.16 Basic control scheme designed for the FC/TCR topology of the example.
                      As expected, the effective reactance of the SVC is a function of the firing angle a.
                      Equation 8.9 may be used to plot Q SVC (a) and to determine the angle a for which
                      Q SVC (a)   0, using the following fundamental relationship

                                         Q SVC ˆ V 2     X C [2p   a ‡ sin 2a]   pX L    (8:10)
                                                 bus
                                                             pX C X L
                      As indicated by Equation 8.10, Q SVC takes a value of zero when the effective
                      reactance X SVC is extremely large, i.e. infinite. This condition is satisfied when the
                      following relationship approaches zero
                                            X C [2(p   a) ‡ sin 2a]   pX L ! 0           (8:11)
                      With the SVC parameters used in this example, the value of the firing angle a that
                      satisfies Equation 8.11 is found to be a   115 . This angle is used as the initial

                      condition for a in the open-loop control of the SVC.
                        To illustrate the SVC's ability to provide voltage regulation at the point of con-
                      nection, a simplified control scheme has been implemented for the single-phase SVC
                      circuit shown in Figure 8.14. The block diagram is shown in Figure 8.16. This control
                      scheme works as follows: The amplitude of the bus voltage V bus is measured and
                      filtered. Then it is compared against the voltage reference V ref . The voltage difference
                      (error) between the two signals is processed by a PI controller which causes a
                      corresponding change in the firing angle a. The value provided by the PI controller
                      is used as the input to the TCR firing angle control unit where the firing pulse is
                      calculated. The zero-crossing of the V bus voltage signal is taken as the reference for
                      the firing angle. Figures 8.17 and 8.18 show the digital implementation of the power
                      circuit and control scheme respectively. Both diagrams were developed using
                      PSCAD/EMTDC v3.04 for PCs.
                        Two experiments are carried out as follows:
                      In experiment 1 the constant AC voltage source V S feeds Load 1 only. The SVC is
                      connected in parallel with the load and it is controlled in open-loop mode. The firing
                      angle a for the thyristors is set at 115 . As mentioned above, with a ˆ 115 the


                      power exchange between the SVC and the AC system is close to zero for the SVC
                      parameters and load conditions shown in Figure 8.17. The voltage V rms at the load
                      point is close to 0.96 p.u. At a time t ˆ 0:6s, Load 2 is switched on by closing Brk,
                      with the load overall increasing. Under the new load conditions the voltage at the
                      load point drops by as much as 16%, giving a V rms value equal to 0.8 p.u., as shown
                      in Figure 8.19(a).
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