
296 CHAPTER 5 Synchronous Machines
theorem applies. From a Thevenin-theorem viewpoint, an open-circuit test gives
the intemal voltage, and a short-circuit test gives information regarding the inter-
nal impedance. From the more specific viewpoint of electromechanical machinery,
an open-circuit test gives information regarding excitation requirements, core losses,
and (for rotating machines) friction and windage losses; a short-circuit test gives in-
formation regarding the magnetic reactions of the load current, leakage impedances,
and losses associated with the load current such as
I2R
and stray load losses. The
only real complication arises from the effects of magnetic nonlinearity, effects which
can be taken into account approximately by considering the machine to be equiv-
alent to an unsaturated one whose magnetization curve is the straight line
Op
of
Fig. 5.9 and whose synchronous reactance is empirically adjusted for saturation as
in Eq. 5.29.
In many cases, synchronous machines are operated in conjunction with an ex-
ternal system which can be represented as a constant-frequency, constant-voltage
source known as an
infinite bus.
Under these conditions, the synchronous speed is
determined by the frequency of the infinite bus, and the machine output power is
proportional to the product of the bus voltage, the machine internal voltage (which is,
in tum, proportional to the field excitation), and the sine of the phase angle between
them (the power angle), and it is inversely proportional to the net reactance between
them.
While the real power at the machine terminals is determined by the shaft power
input to the machine (if it is acting as a generator) or the shaft load (if it is a motor),
varying the field excitation varies the reactive power. For low values of field current,
the machine will absorb reactive power from the system and the power angle will
be large. Increasing the field current will reduce the reactive power absorbed by the
machine as well as the power angle. At some value of field current, the machine power
factor will be unity and any further increase in field current will cause the machine
to supply reactive power to the system.
Once brought up to synchronous speed, synchronous motors can be operated quite
efficiently when connected to a constant-frequency source. However, as we have seen,
a synchronous motor develops torque only at synchronous speed and hence has no
starting torque. To make a synchronous motor self-starting, a squirrel-cage winding,
called an
amortisseur
or
damper winding,
can be inserted in the rotor pole faces,
as shown in Fig. 5.31. The rotor then comes up almost to synchronous speed by
induction-motor action with the field winding unexcited. If the load and inertia are
not too great, the motor will pull into synchronism when the field winding is energized
from a dc source.
Altematively, as we will see in Chapter 11, synchronous motors can be oper-
ated from polyphase variable-frequency drive systems. In this case they can be easily
started and operated quite flexibly. Small permanent-magnet synchronous machines
operated under such conditions are frequently referred to as
brushless motors
or
brushless-dc motors,
both because of the similarity of their speed-torque character-
istics to those of dc motors and because of the fact that one can view these motors
as inside-out dc motors, with the commutation of the stator windings produced elec-
tronically by the drive electronics.