Page 417 - Handbook of Electrical Engineering
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406    HANDBOOK OF ELECTRICAL ENGINEERING

                          Table 15.2. Variation of harmonic coefficients with the commutation angle u

              Harmonic               Magnitude of the coefficient b n at different values of u in degrees
              number
              u           0.01      0.25     1.0       5.0     10.0      20.0     40.0      60.0
              1           1.0       1.0      1.0       1.0      1.0       1.0      1.0       1.0
              5           0.2001    0.2001   0.2001    0.1986   0.1941    0.1766   0.1152    0.0400
              7           0.1429    0.1429   0.1429    0.1409   0.1345    0.1106   0.0384    0.0204
              11          0.0911    0.0910   0.0910    0.0878   0.0779    0.0449   0.0156    0.0083
              13          0.0771    0.0771   0.0771    0.0732   0.0618    0.0262   0.0171    0.059
              17          0.0591    0.0590   0.0590    0.0540   0.0398    0.0035   0.0035    0.035
              19          0.0529    0.0529   0.0529    0.0473   0.0320    0.0028   0.0028    0.0028
              23          0.0438    0.0438   0.0438    0.0370   0.0199    0.0085   0.0055    0.0019
              25          0.0403    0.0403   0.0403    0.0331   0.0153    0.0088   0.0031    0.0016
              29          0.0349    0.0349   0.0344    0.0266   0.080     0.0066   0.0023    0.0012
              31          0.0326    0.0327   0.0327    0.0239   0.0052    0.0047   0.0031    0.0011


                    The near-rectangular line currents will produce volt-drops in the series resistance-reactance
              cables, overhead lines and transformers. These volt-drops will be non-sinusoidal and will distort the
              waveform at their intermediate points of connection. At such points there may be a switchboard or
              distribution board and the loads connected to them will experience the distorted voltage waveform.

                    The line voltage waveform at the primary terminals of the transformer that feeds the bridge
              will be distorted by the short commutation pulses. These are often called ‘notches’. At the thyristors
              or diodes the notches have a near-zero base due to the temporary short circuit during the commutation.
              Immediately upstream of these elements is the impedance of the transformer, and beyond that the
              impedance to the main source of supply. A potential divider circuit exists between the bridge elements
              and the source of supply. Consequently the higher the transformer impedance the lower will be the
              impact of the commutation notches. Suppose the bridge is fed from a motor control centre that has its
              own feeder transformer. Since the feeder transformer and its upstream circuit has a finite impedance,
              there will be a certain amount of distortion to the voltages at the busbars of the motor control
              centre. The notching distortion injects high frequency currents into all the loads and instrumentation
              connected to the busbars. In many situations the loads are not sensitive to this form of distortion, but a
              few in a particular situation may be adversely affected, especially power factor correction capacitors
              and capacitors in fluorescent light fittings (if fitted). Retrofitting filters to an existing set of loads
              on a switchboard or motor control centre may be a difficult task to complete satisfactorily. Some
              instrumentation within or supplied from the switchgear may be requiring timings pulses or triggering
              signals that are derived from the busbar voltages. These signals may be disrupted by the presence of
              notching distortion.
                    The presence of high frequency harmonics in the power supply lines leaving the switchgear
              can cause mutual coupling to electronic and telecommunication cables if they are routed in close
              proximity to the power cables. This can occur especially if the cable racks run parallel to each other
              over an appreciable distance. As a ‘rule-of-thumb’ guide, derived from Table 13.1, the spacing (d)
              between power and electronic cables should be at least,

                                            d ≥ 300 + 1.75I n millimetres

              Where I n is the current rating of the power cable.
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