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                                                             Power electronic control in electrical systems 49

                        Some of the generators in a large system may be operated at light load in a state of
                      readiness or `spinning reserve', in case the system load increases suddenly by a large
                      amount. This can happen, for example, at the end of television transmissions when
                      the number of viewers is exceptionally high.

                      2.8.1   Relationships between power, reactive power, voltage
                              levels and load angle

                      The phasor diagram for the system in Figure 2.16 is shown in Figure 2.17, assuming
                      that the load has a lagging power factor angle f. The line or cable is represented by
                      its impedance R s ‡ jX s , and R s is again neglected (being usually much smaller than
                      X s ). The voltage drop across the transmission line is jX s I, which leads the phasor I by
                      90 . The angle between E s and E r is the load angle, d and

                                   E s cos d ˆ E r ‡ X s I sin f  and  E s sin d ˆ X s I cos f  (2:17)

                      Also
                                         P ‡ jQ ˆ E r I ˆ E r I cos f ‡ jE r I sin f     (2:18)

                      From this we get the power flow equation

                                                        E s E r
                                                    P ˆ     sin d                        (2:19)
                                                         X s
                      and the reactive power equation for the receiving end
                                                        E s cos d   E r
                                                 Q r ˆ E r                               (2:20)
                                                             X s
                      Evidently P ˆ P s ˆ P r as long as the transmission losses are negligible. At the
                      sending end,
                                        P s ‡ jQ s ˆ E s I cos(f ‡ d) ‡ jE s I sin(f ‡ d)  (2:21)























                      Fig. 2.17 Phasor diagram for Figure 2.16.
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