Page 154 - Rashid, Power Electronics Handbook
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10  Diode Recti®ers                                                                                 143

                 where V is the effective (rms) value of the ac component of  The poor TUF of a half-wave recti®er signi®es that the
                        ac
                 load voltage v ,                                     transformer employed must have a 3.496 (1=0.286) VA
                             L
                                                                      rating in order to deliver 1 W dc output power to the load.
                                         q 
                                                 2
                                            2
                                   V ¼    V ÿ V dc            ð10:24Þ  In addition, the transformer secondary winding has to carry a
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                                     ac
                                                                      dc current that may cause magnetic core saturation. As a
                                                                      result, half-wave recti®ers are used only when the current
                 Substituting Eq. (10.24) into Eq. (10.23), the ripple factor can
                                                                      requirement is small.
                 be expressed as
                                                                        In the case of a full-wave recti®er with a center-tapped
                                                                      transformer, the circuit can be treated as two half-wave
                                   s 
                                          2
                                      V L       p      recti®ers operating together. Therefore, the transformer
                                                   2
                              RF ¼        ÿ1 ¼   FF ÿ 1       ð10:25Þ  secondary VA rating V I is double that of a half-wave recti®er,
                                      V dc                                              s s
                                                                      but the output dc power is increased by a factor of four due to
                                                                      the higher recti®cation ratio as indicated by Eqs. (10.5) and
                 In the case of a half-wave recti®er,
                                                                      (10.15). Therefore, the TUF of a full-wave recti®er with center-
                                       p           tapped transformer can be found from Eq. (10.32)
                                            2
                         Half-wave RF ¼  1:57 ÿ 1 ¼ 1:21      ð10:26Þ
                                                                                                  4   0:318 2
                 In the case of a full-wave recti®er,                            Full-wave TUF ¼
                                                                                                2   0:707   0:5
                                      p 
                                           2
                         Full-wave RF ¼  1:11 ÿ 1 ¼ 0:482     ð10:27Þ                         ¼ 0:572              ð10:33Þ
                 10.2.3.6 Transformer Utilization Factor              The bridge recti®er has the highest TUF in single-phase
                 The transformer utilization factor (TUF), which is a measure  recti®er circuits because the currents ¯owing in both the
                 of the merit of a recti®er circuit, is de®ned as the ratio of the  primary and secondary windings are continuous sinewaves.
                 dc output power to the transformer volt-ampere (VA) rating  By substituting Eqs. (10.5), (10.15), (10.29), and (10.31) into
                 required by the secondary winding,                   Eq. (10.28), the TUF of a bridge recti®er can be found
                                         P dc  V I                                               2
                                               dc dc
                                  TUF ¼     ¼                 ð10:28Þ                        0:636
                                        V I    V I                            Bridge TUF ¼           ¼ 0:81        ð10:34Þ
                                          s s   s s                                       0:707   0:707
                 where V and I are the rms voltage and rms current ratings of
                             s
                        s
                 the transformer secondary                            The transformer primary VA rating of a full-wave recti®er is
                                                                      equal to that of a bridge recti®er because the current ¯owing
                                       V m                            in the primary winding is also a continuous sinewave.
                                  V ¼ p ¼ 0:707 V m           ð10:29Þ
                                        
                                   s
                                        2
                                                                      10.2.3.7 Harmonics
                 The rms value of the transformer secondary current I is the  Full-wave recti®er circuits with resistive load do not produce
                                                              s
                 same as that for the load current I . For a half-wave recti®er, I s  harmonic currents in their transformers but they are produced
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                 can be found from Eq. (10.14)                        in half-wave recti®ers. The amplitudes of the harmonic
                                                                      currents of a half-wave recti®er with resistive load, relative
                                              0:5 V m                 to the fundamental, are given in Table 10.1. The extra loss
                                 Half-wave I ¼                ð10:30Þ
                                           s
                                                R                     caused by the harmonics in the resistively loaded recti®er
                                                                      circuits is often neglected because it is not high compared with
                 For a full-wave recti®er, I is found from Eq. (10.16).  other losses. However, with nonlinear loads, harmonics can
                                      s
                                                                      cause appreciable loss and other problems such as poor power
                                             0:707 V m
                                 Full-wave I ¼                ð10:31Þ  factor and interference.
                                          s
                                                R
                 Therefore, the TUF of a half-wave recti®er can be obtained by
                                                                      TABLE 10.1  Harmonic percentages of a half-wave recti®er with resistive
                 substituting Eqs. (10.3), (10.13), (10.29), and (10.30) into Eq.
                                                                      load
                 (10.28).
                                                                      Harmonic   2nd   3rd   4th   5th   6th    7th   8th
                                         0:318 2
                        Half-wave TUF ¼          ¼ 0:286      ð10:32Þ    %       21.2   0    4.2    0     1.8   0     1.01
                                       0:707   0:5
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