[James_H._Harlow]_Electric_Power_Transformer_Engin(BookSee.org)
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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