Patent Application
20110241757
This disclosure relates to electrical power distribution, and in particular, to controlling the complex power vectors in a power transmission system.
The waveform that exists at all points in a power transmission system is ideally a sinusoid of constant frequency. In the US, that frequency is 60 Hz. However, in many parts of the world, the frequency is 50 Hz.
In practice, the waveform that exists in some parts of the power transmission system is a superposition of a fundamental frequency and various harmonic components. These harmonic components arise from various non-linear loads attached to the power transmission system.
The power transmitted by a power transmission system is represented by a power vector in the complex plane. The imaginary component of the power vector represents reactive power, while the real component represents the power that is actually transmitted. The ratio between the real component of the power vector and the magnitude of the power vector is referred to as a “power factor.”
Although the reactive power is not actually transmitted, it nevertheless results in ohmic losses. As a result, if efficient power transmission is sought, it is best to cause the power vector to be purely real. Expressed differently, to transmit power effectively, it is best to cause the power factor to be as close to unity as possible.
The relative magnitudes of the real and reactive power depend on a phase relationship between the voltage and current waveform on the transmission line. This phase relationship depends on the imaginary part of the impedance (i.e. the reactance) seen by the transmission line. Thus, to control the phase relationship, one controls the reactance.
Control over reactance is carried out by monitoring the angle of the power vector and switching reactive elements in and out of electrical connection with the power transmission system, in an attempt to drive the angle back to zero relative to the positive real axis. Depending on whether one wishes to rotate the power vector clockwise or counter-clockwise, one would switch in a capacitative reactance or an inductive reactance. The device for carrying out this function is a static VAR compensator.
In one aspect, the invention features a method of controlling a static VAR compensator. The method includes providing a static VAR compensator having a reactive component and a thyristor for switching the reactive component into and out of a power distribution network; monitoring a periodic waveform on the power distribution network, the waveform including harmonic frequency content; and controlling operation of the thyristor on the basis of the harmonic content of the waveform.
Practices of the invention include those in which controlling operation of the thyristor includes applying a current to a gate of the thyristor when a probability of ringing in a current between an anode of the thyristor and a cathode of the thyristor is in excess of a selected threshold, and those in which controlling operation of the thyristor includes controlling operation on the basis of an estimate of a ratio between a fundamental frequency component of the periodic waveform and the harmonic frequency content.
In one practice, controlling operation of the thyristor includes determining an envelope defined by a superposition of a fundamental frequency component of the periodic waveform and harmonic frequency content of the periodic waveform. Certain of these practices further include, at a first time, turning on current to a gate terminal of the thyristor, the first time being a time at which the envelope reaches a first designated value; and at a second time, turning off current to the gate terminal, the second time being the next time after the first time that the envelope reaches a second designated value.
Other practices include those in which controlling operation of the thyristor includes applying a gate current to the thyristor when the periodic waveform reaches a first designated value, those in which controlling operation of the thyristor includes ceasing application of a gate current to the thyristor when the periodic waveform reaches a second designated value, and those in which controlling operation of the thyristor includes applying a gate current to the thyristor when the periodic waveform reaches a first designated value, and ceasing application of the gate current when the periodic waveform next reaches the designated value, and those in which controlling operation of the thyristor includes causing a gate current to switch between an on-state and an off-state when the periodic waveform reaches a zero crossing.
Other practices of the invention include determining an envelope of the periodic waveform, and controlling operation of the thyristor on the basis of the envelope.
Yet other practices include inspecting a table. In some of these practices, controlling operation of the thyristor includes: determining harmonic frequency content of the periodic waveform, inspecting a table to determine an envelope associated with the harmonic frequency content, and controlling operation of the thyristor on the basis of the envelope.
Other ways of controlling operation of the thyristor are contemplated as being within the scope of this invention. For example, practices of the invention include those in which controlling operation of the thyristor includes applying a gate current to the thyristor at least twice during a period of the periodic waveform; those in which controlling operation of the thyristor includes ceasing application of a gate current to the thyristor at least twice during a period of the periodic waveform; those in which controlling operation of the thyristor includes, on the basis of the periodic waveform, applying gate current during a refractory period of the thyristor, and ceasing application of the gate current during a non-refractory period of the thyristor; those in which controlling operation of the thyristor includes applying gate current symmetrically about time at which the periodic waveform crosses a designated value; and those in which controlling operation of the thyristor includes applying gate current symmetrically about a zero-crossing of the periodic waveform.
In other practices of the invention, controlling operation of the thyristor includes determining a first curve based on a first phase relationship between the harmonic frequency content and a fundamental frequency component of the periodic waveform; and determining a second curve based on a second phase relationship between the harmonic frequency content and the fundamental frequency component, the first and second curve defining an envelope therebetween. Among these practices are those that include applying a gate current to cause a gate pulse that extends from when the first curve crosses a first designated to when the second curve crosses a second designated value.
In another aspect, the invention features a VAR corrector for a power distribution network. The static VAR corrector includes a capacitative reactive load; a thyristor for causing the reactive load to be switched into and out of the power distribution network; a current source for applying a gate current to the thyristor; and a controller for causing gate current to be applied and removed on the basis of harmonic frequency content of a waveform on the network.
In yet another aspect, the invention features a static VAR corrector for a power distribution network. The static VAR corrector includes a capacitative reactive load; a thyristor for causing the reactive load to be switched into and out of the power distribution network; means for applying a gate current to the thyristor; and means for causing gate current to be applied and removed on the basis of a waveform on the network.
These and other features of the invention will be apparent from the following detailed description and the accompanying figures, in which:
A typical static VAR compensator 10, shown in
The thyristor 12 has three terminals: a gate, a cathode, and an anode. When current is applied to the gate, a conducting path exists between the cathode and the anode. This conducting path exists even if current is taken away from the gate. As a result, the thyristor 12 latches into a conducting state. Once it begins to conduct, it continues to do so without the need to continuously provide gate current.
As a result of the conducting path, current begins to flow between cathode and anode. This places the reactive element in communication with the power transmission system and thereby alters the impedance presented to the system. When the correct reactance is switched into the circuit at the correct time, the power vector rotates toward the positive real axis, thus bringing the power factor closer to unity. Alternatively, switching the correct reactance into the circuit at the correct time can reduce the voltage dip and/or flicker.
The thyristor 12 continues to conduct until the current from anode to cathode drops below a threshold. This threshold is slightly above zero amps, but for most practical purposes, is treated as zero amps. Once this value is reached, the conducting path between anode and cathode disappears. The disappearance of this conducting path in turn disconnects the reactance from the circuit.
As the conducting path disappears, charge carriers (i.e. holes and electrons) still present within the thyristor 12 recombine. The time during which this recombination occurs is the “turn-off time,” or “refractory period.” After the refractory period, it becomes safe to turn the thyristor 12 on again.
During the refractory period, the thyristor 12 is particularly vulnerable to damage. If, during the refractory period, the current between anode and cathode were to somehow rise above the threshold, even momentarily, the conducting path could spontaneously re-open, even when no gate current has been applied. This spontaneous and uncontrolled re-opening of the conducting path between anode and cathode can result in serious physical damage to the thyristor 12.
In operation, one would apply a current pulse to the thyristor gate when the current waveform becomes positive. Then, when the current waveform drops to zero, the thyristor 12 would spontaneously stop conducting. Once the current waveform becomes positive again, one would repeat the cycle.
As mentioned above, the current waveform often includes one or more harmonic components, collectively referred to as “harmonic content,” that arise from non-linear loads. To some extent, these harmonics can be minimized by conventional detuning using the inductive reactor 15 shown in
When harmonic content is superimposed on the fundamental, it is possible for the current to momentarily dip below zero, and to then to rise above zero again in a very short time. This effect, which is hereafter referred to as “ringing,” would most likely occur at around the time the fundamental current waveform crosses the time axis. However, although it is possible to predict when this crossing occurs, it is difficult to predict how far away from this crossing one must be before ringing is unlikely to occur.
As noted above, if, as a result of ringing, current momentarily rises above the threshold during a refractory period, the thyristor may sustain serious damage. Consequently, it is preferable to avoid having a refractory period occur while ringing is likely.
In
Knowing when the zero-crossing will occur is of particular importance in a static VAR compensator 10 because it is around that time that ringing due to harmonics is most likely to occur. As noted above, if ringing occurs when the gate current is off, the conducting path may spontaneously re-open during the refractory period, thus raising the risk of thyristor damage. However, as is apparent from
One way to reduce the likelihood of thyristor damage from uncontrolled ringing is to have a pulse of gate current (a “gate pulse” 35) that lasts for at least half a period of the current waveform, as shown in
A difficulty with this approach is that it wastes considerable amounts of energy, and generates excessive waste heat. In principle, the gate current is only needed to open a conducting path between anode and cathode, not to maintain it. In fact, one of the advantages of a thyristor 12 is that once on, it stays on until current drops below a threshold, after which it spontaneously turns off. By having to maintain a gate current for well over half a period, one eviscerates a principal advantage of a thyristor 12.
Another disadvantage is that the timing of the gate current is, to a great extent, an educated guess. It is possible for the gate current to be removed even though ringing is still possible. This risk can be reduced by detuning. But as noted above, detuning can be a difficult procedure.
An alternative approach, which avoids the foregoing difficulties, is to apply a gate pulse 35 symmetrically around each zero-crossing, whether the crossing is a positive crossing (i.e. the waveform is transitioning from being negative to being positive) or a negative crossing.
As shown in
In one embodiment, shown in
In some embodiments, the controller 38 determines the harmonic content of the current and adaptively controls when the gate pulse should occur. In other embodiments, the controller 38 observes the waveform and attempts to predict when zero-crossings will occur.
One way to determine how wide the pulse should be based on harmonic content of the current waveform is to use a table corresponding to the graph shown in
To use the graph shown in
In
The waveforms shown in
While the foregoing discussion has referred to “current waveform,” it will be apparent that current waveform is related to other electrical waveforms, such as voltage and power waveforms, and that the methods described herein can readily be adapted to such waveforms by minor modifications.
