GENERATORS AND POWER CONTROL
Asynchronous
Generators
The
type of generator used in a
If we mechanically spin the shaft of an asynchronous generator so that its rotor spins at exactly the synchronous speed of the grid, nothing will happen. This is because the magnetic field would be rotating at exactly the same speed as the rotor, thereby producing no electricity by induction in the rotor to interact with the stator. However, if we apply more torque to increase the shaft’s rotational speed, the rotor moves a little bit faster than the rotating magnetic field being produced by the stator, which will induce a strong current in the rotor. The harder the shaft is cranked, the more electricity produced. The difference between the rotational speed at peak power and at idle is very small, only about one percent. If the shaft of an asynchronous generator is cranked at slower rotational speeds than the synchronous speed of the grid, the generator will operate as a motor, pulling power from the grid to increase the shaft’s spin to the synchronous speed. Because these generators can turn into motors if insufficient spin is applied to the shafts, they must be disconnected from the grid when their rotational speeds are not fast enough to produce usable power.
Although the generators
and rotors can be any size as long as they are matched to each other and to
the water velocity, we should perhaps make a few assumptions to provide
examples of what is possible. If we
assume that each turbine has a rated capacity of 600 kW, the generators used in
the Gulf Stream Turbine could be virtually identical to those used in the Nordex N43/600 kW wind-driven system. These machines use generators of two
types. They use a single wound 4-poler
asynchronous 600 kW generator, or a double wound 4/6-pole asynchronous
generator. Although the Nordex literature states that the synchronous speeds are
1,500 rpm for their 4-pole generators and 1,000 rpm for their 6-pole
generators, these speed are based on the 50 Hz current
that is used in
The speed of the rotors and the number of magnetic lines per pole fix the magnitude of the voltage generated. The more poles there are, the more lines of magnetic force. This also means that the more poles there are, the lower the rpm required to produce the same amount of power at the same frequency. The following formula can be used to calculate the rpm required to generate electricity of with differing numbers of poles:
rpm = (C x 60) / ( P / 2) C = frequency in cycles per second
P = the number of poles (an even number)
Conventional wind-powered machines have compact
generators that have 4 or 6 poles and use a rotor-gearbox-generator drive
train. The Lagerway wind machines, made in
Power Control for Asynchronous
Generators
A
problem can be caused by the water having too much velocity for what a turbine
power plant, equipped with asynchronous generators, can safely handle. If the generators should be overpowered by an
extremely strong current so that it is forced to rotate too fast to remain in
sync with the grid’s 60-cycle current, serious damage can occur.
As the water current
velocity increases, the generator’s rotational speed can be controlled to some
degree by increasing the strength of the electrical current in the stator to
increase the strength of the magnetic field.
Beyond that, there could be a need for limiting the power input to the
generator. Because wind turbines have
this problem, we should look at the systems that they use. They use both pitch controlled and stall
controlled systems.
On a pitch controlled wind turbine the turbine’s electronic controller
checks the power output of the turbine several times per second. When the power output becomes too high, it
sends an order to the blade pitch mechanism, which immediately turns the rotor
blades slightly out of the wind.
Conversely, the blades are turned back into the wind whenever the wind
drops. On a pitch controlled wind
turbine, a computer changes the pitch of the blades a few degrees every time
the wind changes to keep the rotor blades at the optimum angle to maximize
output for all wind speeds. Because of
its complexity, the pitch-controlled system might not be the best choice for
the
The
stall controlled wind turbines have
rotor blades that are bolted onto the hub at a fixed angle. The geometry of the rotor blade profile has
been aerodynamically designed to ensure that the moment the wind speed becomes excessive, it creates turbulence on the side of the rotor
blade that is away from the wind. This
produces a stall that prevents the lifting force of the rotor blade from acting
on the rotor. As the wind speed
increases, the angle of attack of the rotor blade increases until at some point
the blade starts to stall. On the stall
corrected wind turbines, the blade twists slightly along its longitudinal axis. This is partly to ensure that the rotor blade
stalls gradually rather than abruptly when the wind speed reaches its critical
value. The stall control systems present
a very complex aerodynamic design problem.
Around two thirds of the wind turbines currently being installed in the
world are of this type. Because the
stall-controlled system has no moving parts or complicated control system to
break or malfunction, it should be considered for those submersible turbines
that will be placed where the current’s velocity may occasionally become
excessive for the generators. A reason
not to use the stall corrected system is that, as the blades stall, there would
be a substantial increase in drag, which would pull the machines down to
greater depths and could put an excessive strain on the anchoring system.
Another method for controlling the power input to the asynchronous generator would be to have a fluid coupling or a magneto-rheological fluid clutch on the high-speed shaft, between the gearbox and the generator, that would allow some slippage, with no mechanical wear, should the power input become excessive. This slippage can be controlled by the power output of the generator. Because the slippage would generate heat, a system to cool the fluid would be required.
A rather drastic approach to preventing damage to generating units in unusually strong currents would be to simply shut off the current from the grid to the generator’s stator. Cutting off this current would eliminate the magnetic forces that induce the electricity in the spinning armature. The turbine and generator could then spin harmlessly at high speeds while producing no power.
Because
of the relative uniformity of a current’s velocities, it is possible that no
power-limiting device will be required.
Another approach to solving the
problems caused by variations in current strength is to use variable-speed
generators that have indirect hookups
to the grid. Instead of using an
asynchronous generator that has its rotational speed controlled by the 60 Hz
cycles of the grid, the variable-speed generator runs on its own, on a separate
mini AC-grid. This grid is controlled
electronically (using an inverter) so that the frequency of the alternating
current in the stator of the generator may be varied. In this way it is possible to run the turbine
and generator at variable rotational speeds.
The turbine generates alternating current at the variable frequency
applied to the stator; then the current is converted electronically to direct
current; then back again to AC with the frequency in sync with the grid. Theoretically, the variable speed generator
offers an advantage in terms of annual production for the wind-powered turbines
because it is possible for them to run at an optimal rotational speed,
depending on the wind velocity. Using
the variable-speed generator for the water-powered turbines would avoid those
problems that could otherwise be caused by an excessively strong current
overpowering an asynchronous generator – as well as permit the
production of usable power from rotation speeds that are too slow for the
asynchronous generator. A negative for
the variable-speed generator is that they have more complicated electronics
that could cause service problems.