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Closing resistance Rs to limit overvoltage to 1.8 pu

Short answer

Insert 34.7 Ω as the switching resistor in series during closing. With total circuit resistance 44.81 Ω, the maximum overvoltage is limited to 1.8 pu.

Using the single phase equivalent lumped parameter model circuit of 3-phase, 400kV, 50Hz, 400 km long EHV line shown below, compute the switching resistance Rs to be inserted during the closing of circuit breaker so that maximum switching overvoltage will be limited to 1.8 pu. [Figure: source Vs with 0.12 Ω internal resistance feeds circuit breaker CB; resistor Rs with its own switch is connected in parallel with CB; series line impedance 10 Ω + 0.5 H to receiving node Vo; shunt capacitor 5 μF from Vo to ground]

When the breaker closes, the line acts as a series R–L–C circuit excited by a step voltage EE (closing at the peak of the source voltage, 1 pu). With no trapped charge, the capacitor voltage is

vC(t)=E[1−e−αtα2+ω2ωcos⁡(ωt−ϕ)],α=R2L, ω=1LC−α2v_C(t) = E\left[1 - e^{-\alpha t}\frac{\sqrt{\alpha^2+\omega^2}}{\omega}\cos(\omega t - \phi)\right], \quad \alpha = \frac{R}{2L},\ \omega = \sqrt{\frac{1}{LC} - \alpha^2}

Setting dvC/dt=0dv_C/dt = 0 gives sin⁡ωt=0\sin\omega t = 0, so the first (largest) peak is at t=π/ωt = \pi/\omega:

Vmax=E(1+e−απ/ω)V_{max} = E\left(1 + e^{-\alpha\pi/\omega}\right)

Data: L=0.5L = 0.5 H, C=5 μC = 5\ \muF. Total resistance R=0.12+10+RsR = 0.12 + 10 + R_s (source + line + switching resistor in series during closing).

ω0=1LC=10.5×5×10−6=632.46 rad/s\omega_0 = \frac{1}{\sqrt{LC}} = \frac{1}{\sqrt{0.5 \times 5\times10^{-6}}} = 632.46\ \text{rad/s}

Without RsR_s (for reference)

R=10.12 ΩR = 10.12\ \Omega, so α=10.12/(2×0.5)=10.12 s−1\alpha = 10.12/(2\times0.5) = 10.12\ \text{s}^{-1} and ω=632.37\omega = 632.37 rad/s.

Vmax=1+e−10.12π/632.37=1+0.951=1.951 puV_{max} = 1 + e^{-10.12\pi/632.37} = 1 + 0.951 = 1.951\ \text{pu}

Required RsR_s for 1.8 pu

1+e−απ/ω=1.8e−απ/ω=0.8αω=ln⁡(1/0.8)π=0.22314π=0.07103\begin{aligned} 1 + e^{-\alpha\pi/\omega} &= 1.8 \\ e^{-\alpha\pi/\omega} &= 0.8 \\ \frac{\alpha}{\omega} &= \frac{\ln(1/0.8)}{\pi} = \frac{0.22314}{\pi} = 0.07103 \end{aligned}

Using ω2=ω02−α2\omega^2 = \omega_0^2 - \alpha^2:

ω=ω01+(α/ω)2=632.461+0.071032=630.87 rad/sα=0.07103×630.87=44.81 s−1R=2Lα=2×0.5×44.81=44.81 ΩRs=44.81−10−0.12=34.69 Ω\begin{aligned} \omega &= \frac{\omega_0}{\sqrt{1 + (\alpha/\omega)^2}} = \frac{632.46}{\sqrt{1 + 0.07103^2}} = 630.87\ \text{rad/s} \\ \alpha &= 0.07103 \times 630.87 = 44.81\ \text{s}^{-1} \\ R &= 2L\alpha = 2 \times 0.5 \times 44.81 = 44.81\ \Omega \\ R_s &= 44.81 - 10 - 0.12 = 34.69\ \Omega \end{aligned}

Check: with R=44.81 ΩR = 44.81\ \Omega, e−44.81π/630.87=0.800e^{-44.81\pi/630.87} = 0.800, so Vmax=1.80V_{max} = 1.80 pu ✓

 Vs ~--0.12--+--CB--+--10 ohm--0.5 H--+-- Vo
             |      |                 |
             +-Rs-/-+               5 uF
                                      |
 -------------------------------------+-- gnd

The resistor is in circuit only for the first few milliseconds (the pre-insertion time). The main contacts then short it out, which produces a second, smaller transient.

Answer: Rs≈R_s \approx 34.7 Ω (total circuit resistance 44.81 Ω), assuming no trapped charge and closing at the voltage peak.

✓ Answer checked by Claude Opus 5.5 (high effort)

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