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ate of rise of transient-recovery voltage can also occur. It is recommended that a TRV study be conducted<br />

prior to selection of a circuit breaker and/or prior to installation of a current-limiting reactor.<br />

2.9.5.2 Circuit-Breaker TRV Capabilities<br />

Rated circuit-breaker TRV capabilities can be obtained from the manufacturer or from various standards<br />

such as ANSI C37.06 [15] or IEC 62271-100. [16] Circuit breaker TRV capabilities are normally defined<br />

by two sets of parameters. One indicates the maximum voltage peak that the circuit breaker can withstand,<br />

and the other one represents the rate of rise of the voltage, i.e., the minimum time to the voltage peak.<br />

Parameters introduced in ANSI C37.06 define the TRV capability of a circuit breaker by means of two<br />

types of envelopes. For circuit breakers rated 123 kV and above, the envelope has an exponential-cosine<br />

shape if the symmetrical short-circuit current is above 30% of the circuit breaker short-circuit capability<br />

(see Figure 2.9.35). At 30% and below, the envelope has a 1-cosine shape. For circuit breakers rated 72.5<br />

kV and below, the envelope has a 1-cosine shape over the entire fault-current range. Circuit breakers are<br />

also required to withstand line-side TRV originating from a “kilometric” or short-line fault (SLF). This<br />

type of TRV normally reaches its peak during the delay time of the source-side TRV (see Figure 2.9.35).<br />

When the actual fault current is less than the circuit-breaker rated fault current, circuit breakers can<br />

withstand higher TRV voltages in a short rise time versus their rated value. As shown in Figure 2.9.35,<br />

when the actual fault current is 60% of rated value, the circuit breaker can withstand a TRV of 7% higher<br />

voltage for a duration 50% shorter than rated time. Therefore when using reactors to reduce the shortcircuit<br />

level at a substation, it might be more beneficial, from the TRV point of view, to install currentlimiting<br />

reactors at the upstream feeding substation, where circuit breakers are rated for higher shortcircuit<br />

level.<br />

2.9.5.3 TRV Evaluation<br />

Computer simulation, or even manual calculation using the current-injection method, can be employed<br />

to evaluate the TRV across the circuit-breaker terminals. IEEE C37.011-1994 [17] also provides some<br />

guidance for evaluating the TRV. To conduct the study, the electrical characteristics of all the equipment<br />

involved in the TRV circuit is required. Equipment characteristics can normally be obtained from the<br />

equipment nameplate. However, stray capacitances or inductances are not normally shown on the<br />

nameplates. To obtain this information, the equipment manufacturer should be consulted. When dealing<br />

with TRV associated with fault current limited by a current-limiting reactor, normally the first pole to<br />

open, during an ungrounded three-phase fault at the terminal, experiences the highest peak of TRV. (For<br />

certain conditions during a two-phase-to-ground fault, higher TRV can be experienced [11]). The shape<br />

of TRV when fault current is limited by a reactor is oscillatory (underdamped) and is very similar to the<br />

TRV generated when fault current is limited by a transformer impedance.<br />

When modeling a reactor for TRV studies, the following items shall be considered:<br />

• All types of reactors have stray capacitances, whose values can be obtained from the manufacturer.<br />

Generally, the stray capacitance of a dry-type reactor is on the order of a few hundred pF and that<br />

of an oil-filled reactor is on the order of a few F (see Figure 2.9.36).<br />

• Reactor losses at power frequency are very small and insignificant. However, as a result of skin<br />

effect and eddy losses at high frequencies (in the range of kHz), the reactor losses are significant<br />

(see Figure 2.9.36).<br />

This characteristic of the reactor can help to damp the transients and shall be reflected in the model<br />

by including a frequency-dependent resistance in series with the reactance.<br />

2.9.5.4 TRV Mitigation Methods<br />

Should the system TRV exceed the circuit breaker capability, one or a combination of the following<br />

mitigation methods can be employed:<br />

1. Installation of a capacitor across the reactor terminals<br />

2. Installation of a capacitor to ground from the reactor terminal connected to the circuit breaker.<br />

For bus-tie reactors, capacitors shall be installed to ground at both reactor terminals.<br />

From a TRV point of view, either of the previous mitigation methods is acceptable. However, from<br />

an economic point of view, it is more cost-effective to install the capacitor between the reactor terminals,<br />

since the steady-state voltage drop across the reactor is significantly lower than the line-to-ground voltage.<br />

Consequently, a lower voltage capacitor can be used.<br />

Figure 2.9.37 shows the result of a TRV study for a subtransmission substation. Curve b in this figure<br />

shows the system TRV prior to installation of a current-limiting reactor. It slightly exceeds the circuit<br />

breaker capability, as seen in Curve a. After installation of a current-limiting reactor, the system TRV<br />

exceeds the circuit breaker capability significantly, as seen in Curve c. To reduce the rate of rise of TRV,<br />

a capacitor was installed across the reactor terminals. As seen in Curve d, the system TRV has been<br />

modified to an acceptable level.<br />

FIGURE 2.9.35 Typical TRV capability envelopes for 123-kV-class circuit breaker at (a) 60% and (b) 100% of rated<br />

fault current.<br />

FIGURE 2.9.36 Reactor model for TRV studies, where: C gl and C g2 = stray capacitance of reactor terminals to<br />

ground, C t = terminal-to-terminal stray capacitance, L = reactor inductance, and R (f) = reactor-frequency-dependent<br />

resistance.<br />

© 2004 by CRC Press LLC<br />

© 2004 by CRC Press LLC

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