Page 413 - Handbook of Electrical Engineering

402 HANDBOOK OF ELECTRICAL ENGINEERING

The use of rectifiers and inverters for variable speed motor drives is becoming common in the
oil industry, especially for large gas compressors and oil pumps. Adding these to an existing power
system can create problems that are difficult to solve, even if they are furnished with harmonic
filters. Power systems that have long high-voltage feeder cables, such as submarine cables between
platforms, are particularly sensitive to harmonic currents created by rectifiers-inverter loads. The
amount of shunt capacitance in these cables can be enough to cause a resonant condition at a low
multiple of the fundamental e.g. 5, 7, 11, 13. These low frequency harmonics usually exist at a
magnitude that cannot be ignored in such situations. This can present the power system engineer
with a difficult task in designing a suitable anti-resonant filter. The remainder of this chapter is
concerned only with harmonics caused by variable speed motor drives.
The theoretical operations of rectifiers and inverters under steady state and transient conditions
are described in many publications, for example References 1 to 6.

Reference 2 also describes the ‘on-off’ characteristics of the power semiconductors used in
the bridges e.g. diodes, thyristors, triads, gate turn-off thyristors and bipolar power transistors. Only
the steady state operations of bridges are described herein. For such operations it is assumed that the
load is well matched to the rating of the bridge. The remainder of this section is an introduction to
the subject of harmonic voltages and currents that are caused by variable speed systems for DC and
AC motors. It emphasises the main aspects that affect the supply power systems.

15.2 RECTIFIERS
15.2.1 Diode Bridges

Power rectifiers rated above a few kVA are usually three-phase units and occasionally six-phase
units. The bridge elements may be diodes, thyristors (silicon controlled rectifiers) or power transistors
operated as switches.

Diode bridges are the simplest and are suitable where the output DC voltage is constant and
related to the input AC voltage by a fixed factor. They are well suited to battery chargers, uninterruptible
power supplies and cathodic protection units. Figure 15.1 shows the basic element of a three-phase
diode bridge, in this case the rectifier elements R 1 to R 6 and diodes, not thyristors as shown.

15.2.1.1 Commutation

The transfer of the load current from one diode to the next is called ‘commutation’. This takes
place when the potential at the anode of the first diode has fallen to a value equal to the rising
potential at the anode of the second diode. Shortly after the transfer is initiated both diodes conduct
the current and a temporary short circuit exists across the two phases supplying the diodes. Since the
short circuit contains the leakage reactance of the supply transformer, plus the impedance upstream
of the transformer, there is sufficient inductance to delay the rise in current in the second diode.
Hence the current rises exponentially from zero to a value equal to the DC load current. At this
point the commutation is complete and the first diode ceases to conduct. The finite time taken by the
commutation process is related to the periodic time of the supply voltage by defining an angle ‘u’
called the commutation angle. As the load current is increased the commutation time is increased
and so the angle u increases. At no-load the angle u is zero. At full-load the angle u is between zero
◦
◦
and 60 for properly designed bridges, and in practice u will be in the order of 10 if a good power
factor is to be obtained, as shown in Table 15.1.