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               58 Power systems engineering ± fundamental concepts

                      average power is V m I m /2, this represents a peak±peak fluctuation 200% of the mean
                      power, at double frequency. The oscillation of power in single-phase circuits con-
                      tributes to lamp flicker and causes vibration in motors and transformers, producing
                      undesirable acoustic noise.

                      2.10.2 Two-phase

                      Suppose we have a two-phase load with phases a and b, with u a ˆ V m cos
                      ot, i a ˆ I m cos (ot   f) and u b ˆ V m sin ot, i b ˆ I m sin (ot   f). This system is said
                      to be balanced, because the voltages and currents have the same RMS (and peak)
                      values in both phases, and their phase angles are orthogonal. The total instantaneous
                      power is now given by

                                   p ˆ u a i a ‡ u b i b
                                     ˆ V m I m [ cos(ot)cos(ot   f) ‡ sin(ot) sin(ot   f)]
                                                                                        (2:32)
                                     ˆ V m I m cos f
                                     ˆ 2VI cos f

                      The oscillatory term has vanished altogether, which means that the power flow is
                      constant, with no fluctuation, and the average power P is therefore equal to the
                      instantaneous power p. Note that if the phases become unbalanced, an oscillatory
                      term reappears.


                      2.10.3   Three-phase
                      Suppose we have a three-phase load as in Figures 2.20 and 2.22, with phases a, b and
                      c, with
                                   u a ˆ V m cos ot      i a ˆ I m cos(ot   f)
                                   u b ˆ V m cos(ot   2p=3) i b ˆ I m cos(ot   2p=3   f)  (2:33)
                                   u c ˆ V m cos(ot ‡ 2p=3)  i c ˆ I m cos(ot ‡ 2p=3   f)
                      This system is said to be balanced, because the voltages and currents have the same
                      RMS (and peak) values in all three phases, and their phase angles are equi-spaced
                      (i.e. with a 120 symmetrical phase displacement). The total instantaneous power is

                      now given by

                          p ˆ u a i a ‡ u b i b ‡ u c i c
                            ˆ V m I m [cos(ot) cos(ot   f) ‡ cos(ot   2p=3) cos(ot   2p=3   f)
                              ‡ cos (ot ‡ 2p=3) cos (ot ‡ 2p=3   f)]
                                                                                        (2:34)
                              3
                            ˆ V m I m cos f
                              2
                            ˆ 3VI cos f
                      As in the two-phase system, the oscillatory term has vanished. The power flow is
                      constant, with no fluctuation, and the average power P is equal to the instantaneous
                      power p. If the phases become unbalanced, an oscillatory term reappears.
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