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Temporary overvoltage for SLG fault at line middle

Short answer

Prefault voltage at midpoint rises to 1.0707 pu by Ferranti effect. With generator grounding impedance 4+j50 Ω and fault impedance j35 Ω, the earth-fault factor is 1.204. The temporary overvoltage on healthy phases is 1.29 pu (≈298 kV rms phase-to-ground).

Compute the temporary over voltage due to single line to ground fault for a 400 kV, 50 Hz, 3 phase, AC transmission line having r = 0.04 Ω/km, l = 1.01 mH/km and C = 11 nF/km if the fault is at the middle of the line. Take fault impedance of j35 Ω, generator grounding impedance 4 + j50 Ω. Take length of line = 400 km.

A single line-to-ground (SLG) fault raises the power-frequency voltage of the healthy phases. On an unloaded long line it is raised further by the Ferranti effect. The result is a temporary overvoltage (TOV).

Method and assumptions (data not given are taken as below and stated):

  1. Generator emf E=1E = 1 pu (phase), with the generator's own sequence impedances neglected (not given).
  2. Prefault voltage at the fault point is found from the long-line equation with the far end open (Ferranti rise):
Ef=E cosh⁡γ(l−x)cosh⁡γlE_f = E\,\frac{\cosh\gamma(l - x)}{\cosh\gamma l}

where xx is the distance of the fault from the source. 3. Positive- and negative-sequence impedance up to the fault: Z1=Z2=(r+jωl) xZ_1 = Z_2 = (r + j\omega l)\,x. 4. Zero-sequence impedance Z0=Z1+3ZnZ_0 = Z_1 + 3Z_n. No separate zero-sequence line data are given, so the line's Z0Z_0 is taken equal to Z1Z_1, and ZnZ_n is the generator neutral impedance.

Healthy-phase voltage for an SLG fault on phase aa through ZfZ_f:

Vb=Ef[a2−Z0−Z12Z1+Z0+3Zf]=Ef[a2−ZnZ1+Zn+Zf]V_b = E_f\left[a^2 - \frac{Z_0 - Z_1}{2Z_1 + Z_0 + 3Z_f}\right] = E_f\left[a^2 - \frac{Z_n}{Z_1 + Z_n + Z_f}\right] Vc=Ef[a−ZnZ1+Zn+Zf],a=1∠120∘V_c = E_f\left[a - \frac{Z_n}{Z_1 + Z_n + Z_f}\right], \qquad a = 1\angle120^\circ

Data: r=0.04 Ωr = 0.04\ \Omega/km, l=1.01l = 1.01 mH/km, C=11C = 11 nF/km, length 400 km, fault at x=200x = 200 km, Zf=j35 ΩZ_f = j35\ \Omega, Zn=4+j50 ΩZ_n = 4 + j50\ \Omega.

Step 1: line constants

z=0.04+j(314.16)(1.01×10−3)=0.04+j0.3173 Ω/kmy=j(314.16)(11×10−9)=j3.456×10−6 S/kmγ=zy=(0.0659+j1.0492)×10−3 /kmβl=1.0492×10−3×400=0.4189 rad=24∘\begin{aligned} z &= 0.04 + j(314.16)(1.01\times10^{-3}) = 0.04 + j0.3173\ \Omega/\text{km} \\ y &= j(314.16)(11\times10^{-9}) = j3.456\times10^{-6}\ \text{S/km} \\ \gamma &= \sqrt{zy} = (0.0659 + j1.0492)\times10^{-3}\ /\text{km} \\ \beta l &= 1.0492\times10^{-3}\times400 = 0.4189\ \text{rad} = 24^\circ \end{aligned}

Step 2: prefault voltage at the midpoint (Ferranti)

Ef=cosh⁡(200γ)cosh⁡(400γ)≈cos⁡12∘cos⁡24∘=0.97810.9135=1.0707 puE_f = \frac{\cosh(200\gamma)}{\cosh(400\gamma)} \approx \frac{\cos 12^\circ}{\cos 24^\circ} = \frac{0.9781}{0.9135} = 1.0707\ \text{pu}

Step 3: sequence impedances

Z1=Z2=200(0.04+j0.3173)=8+j63.46 ΩZ1+Zn+Zf=(8+j63.46)+(4+j50)+j35=12+j148.46 Ωm=ZnZ1+Zn+Zf=4+j5012+j148.46=0.3368∠0.05∘\begin{aligned} Z_1 &= Z_2 = 200(0.04 + j0.3173) = 8 + j63.46\ \Omega \\ Z_1 + Z_n + Z_f &= (8 + j63.46) + (4 + j50) + j35 = 12 + j148.46\ \Omega \\ m &= \frac{Z_n}{Z_1 + Z_n + Z_f} = \frac{4 + j50}{12 + j148.46} = 0.3368\angle0.05^\circ \end{aligned}

Step 4: healthy-phase voltages

Vb/Ef=a2−m=(−0.5−j0.8660)−0.3368=−0.8368−j0.8663∣Vb/Ef∣=1.2044∣Vc/Ef∣=∣(−0.5+j0.8660)−0.3368∣=1.2040\begin{aligned} V_b/E_f &= a^2 - m = (-0.5 - j0.8660) - 0.3368 = -0.8368 - j0.8663 \\ |V_b/E_f| &= 1.2044 \\ |V_c/E_f| &= |(-0.5 + j0.8660) - 0.3368| = 1.2040 \end{aligned}

Step 5: temporary overvoltage

VTOV=1.2044×1.0707=1.290 pu=1.290×4003=297.8 kV (rms, phase)\begin{aligned} V_{TOV} &= 1.2044 \times 1.0707 = 1.290\ \text{pu} \\ &= 1.290 \times \frac{400}{\sqrt3} = 297.8\ \text{kV (rms, phase)} \end{aligned}
QuantityValue
Ferranti factor at mid-line1.0707
Earth-fault factor $a^2 - m
TOV (phase bb)1.290 pu ≈ 297.8 kV

Answer: TOV on the healthy phase ≈ 1.29 pu (≈ 298 kV rms to ground, peak ≈ 421 kV), with the stated assumptions. The ratio Z0/Z1Z_0/Z_1 is high here because of the generator grounding impedance. A lower neutral impedance would reduce the TOV.

✓ Answer checked by Claude Opus 5.5 (high effort)

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