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HARMONIC VOLTAGES AND CURRENTS       413

           Note, a ‘rule-of-thumb’ expression for the power factor is,

                                                       ω o
                                            cos Ø 1   0.7  + 0.2
                                                       ω n
           Where ω o is the running speed of the motor and ω n is the rated speed of the motor.
                 Hence,
                                     400

                      cos Ø 1   0.7 ×     + 0.2
                                     975
                            = 0.4872   which is a little optimistic but a satisfactory estimate.


           15.3 HARMONIC CONTENT OF THE SUPPLY SIDE CURRENTS

           15.3.1 Simplified Waveform of a Six-pulse Bridge

           In a well-designed rectifier-load system the inductance in the DC circuit may be assumed to be
           sufficiently large to completely smooth the DC current. In practice the smoothing is not perfect but
           adequate for the performance of the bridge. In the ideal situation the shape of the current in the three
           lines that supply the bridge are rectangular in shape, when the commutation angle u is assumed to
                                                ◦
           be zero. A positive rectangle of duration 120 is followed by a pause of zero value and a duration of
             ◦
           60 . A second rectangle of negative magnitude follows in the same form as the positive rectangle. In
           this simplified situation only the magnitude of the rectangle changes with loading of the bridge, the
           sides of the rectangles do not change shape or position relative to each other. Hence the harmonic
           components of the AC currents remain constant with loading.
                 For the simplified situation the harmonic coefficients of the AC currents are only odd coeffi-
           cients, and all triple coefficients are absent. The coefficients may be summarised as,

                                    I n  1
                                      =   ,  for n = 5, 7, 11, 13, 17, 19 etc.
                                    I 1  n
                                    n = 6k ± 1

           Where k = 1, 2, 3,..., ∞. The lowest harmonic present is the fifth.
                                                                       ◦
                 For the purpose of Fourier analysis assume that the positive 120 rectangle is placed with the
           centre at π/2onthe x-axis, and the centre of the negative rectangle at 3π/2. The analysis will yield
           only coefficients for the sine terms. Assume the amplitude i max of the rectangle is 1.0. The Fourier
           integration yields the harmonic coefficients as,
                               1      πn       5πn       7πn      11πn
                          b n =    cos    − cos    − cos     + cos        and a n = 0
                               nπ      6        6         6         6
                                  n=∞

                                      b n sin ωt                                         (15.17)
                       i(ωt) = i max
                                  n=1
           Let b n be denoted as b n120 for use in sub-section 15.3.4.

                 The lowest harmonic present is the fifth.
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