Talking about HV shunt reactor switching (1)

HV shunt reactor switching

These notes aim to give basic idea of the main criticalities related to HV shunt reactor switching, particularly in terms of voltage, and how such problems are faced and solved by modern switching technology.

Content:

1. Shunt reactors application
2. Closing operation
3. Opening operation (in next part)
4. Conclusions (in next part)

Shunt reactors application

Three-phase shunt reactors are basically aimed to compensate excess of reactive power generation so preventing unacceptable voltage rise and power losses.

Lightly loaded¹, long power transmission lines over 220kV, or cables 100kV and higher, are capacitive loads causing voltage increase because of the line charging currents flowing through the line / cable self inductance (Ferranti effect).

¹ As a reference value, it should be considered as “light” a load less than 70% of the surge impedance loading (SIL). For instance, a 345kV line with surge impedence 350Ω has about 345²/350 = 340MW SIL.

That is consistent with the fact that in some EHV lines permanently under-loaded, fixed reactors are installed (provided just with a disconnecting switch in presence of redundant shunt reactors, for maintenance purposes).

Another example of shunt reactor application is in presence of filter banks acting as capacitors at power frequency: that is the typical situation of HVDC converter station. HVDC converters produce harmonic distortion that need proper filter design to avoid heavy impact on network power quality.

Different combination of filters could be are foreseen in different load conditions to get the target value of THD. At the same time filters’ capacitor banks act also as a reactive power source providing the needed Mvar to the converter, which is an important inductive load. Sometimes it could happen that specific combinations of converter load and filters configuration can satisfy the harmonic constraints, but lead to the reactive power generated by filters exceeding that consumed by converter over acceptable level: in that situations a shunt reactor is used.

The configuration of shunt reactors may be various (bank of single-phase reactors, three-phase unit with a 3- or 5-legged core, etc.) , but following considerations still remain valid.

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Closing operation

For what concerns the closing operation, the shunt reactor can be simply modeled as an inductance in series with a resistance. The latter is always present, despite the effort to minimize losses.

Energy stored in the inductor before circuit breaker closing is zero, and network voltage is:

The current flowing in the circuit is then:

Where:

The way to cancel the transient term is to close the circuit breaker when the steady state component of current is zero (γ = φ). More simply, suppose and resistive part of the reactor impedance be zero (φ = 90°): the transient part of current is zero if the circuit breaker is switched on when the voltage
reaches its maximum value (γ = 90°).

On the contrary, the transient term will be maximum if the circuit breaker closes with γ = φ ±90°. In the simplified example that means γ = 0.

As the two terms (transient and steady state) sum each other, half a cycle later, when they have the same sign, the current increases over the steady state maximum value. The actual value depends on the circuit damping. Very low damping circuits (it is almost the case of shunt reactors) can see a current doubled, compared with the steady state.

Because of above mentioned asymmetry in the transient current trend, closing operation can also generate zero sequence currents. Despite of the linear design of shunt reactors, in case of their switching in at the worst instant (phase voltage equal to zero), the flux will increase with the voltage-time-area during the first half-cycle to a value twice the maximum flux in normal operation.

The current is proportional to the flux density, until reactor core saturation occurs. Above the point of saturation the current will increase faster than the flux. Saturation will be present in different amount in the three phases, because of the three-phases voltage 120° displacement.

That means the sum of DC components in the three phase currents will not be null, so producing a zero sequence current which could lead to nuisance tripping by protections.

Several manufacturers offer their own models of CSD: basically the principle is the same and it is based on the measuring of voltage upstream the circuit breaker, on the source side. In several cases a current feedback signal is used for adaptation control: as the switching times can be affected by temperature, auxiliary voltage variations, mechanical contingencies, etc. a deviation from target instant can occur. Such deviation is detected and properly taken into consideration during the next operation.

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Continue reading 2nd part of this article

Bibliography

1. “Live Tank CB Application Guide” – ABB
2. “Buyers Guide HV Live Tank Circuit Breakers Ed5 en” – ABB
3. “Trasmissione e distribuzione dell’energia elettrica” – N. Faletti, P. Chizzolini
4. “Switching Shunt Reactors” – Roy W Alexander, NeilA. McCord P.E.
5. “HV shunt reactor secrets for protection engineers”- Zoran Gajić, Birger Hillström, Fahrudin Mekić