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Inductance of 420 kV line, transposed and untransposed

Short answer

Equivalent radius is 8.526 cm. Untransposed: self-inductance 1.1726 mH/km, mutuals 0.2133 and 0.1051 mH/km. Transposed: L_s=1.1726, L_m=0.1772 mH/km, giving positive-sequence inductance L1 = 0.995 mH/km.

For the 3-phase 420 kV horizontal line having conductor diameter of 2 × 3.18 cm and bundle spacing 45.72 cm. The ground clearance is 15 m and phase spacing is 11 m. Calculate the inductance in both un-transposed and transposed condition.

For EHV lines, the inductance matrix is [L]=μ02π[M]=0.2 [M][L] = \dfrac{\mu_0}{2\pi}[M] = 0.2\,[M] mH/km. Here [M][M] is Maxwell's coefficient matrix (image method, equivalent bundle radius; internal flux neglected). Transposition replaces it by averaged self and mutual terms.

Data

  • 420 kV, flat horizontal, S=11S = 11 m, H=15H = 15 m
  • Bundle 2×3.182 \times 3.18 cm diameter, so r=1.59r = 1.59 cm; B=45.72B = 45.72 cm
  • μ0/2π=2×10−7\mu_0/2\pi = 2 \times 10^{-7} H/m =0.2= 0.2 mH/km

Step 1: Equivalent radius

req=rB=1.59×45.72=8.526 cmr_{eq} = \sqrt{rB} = \sqrt{1.59 \times 45.72} = 8.526\ \text{cm}

Step 2: Maxwell coefficients

Mii=ln⁡2Hreq=ln⁡300.08526=5.8632M12=M23=ln⁡112+30211=1.0664M13=ln⁡222+30222=0.5253\begin{aligned} M_{ii} &= \ln\frac{2H}{r_{eq}} = \ln\frac{30}{0.08526} = 5.8632 \\ M_{12} = M_{23} &= \ln\frac{\sqrt{11^2 + 30^2}}{11} = 1.0664 \\ M_{13} &= \ln\frac{\sqrt{22^2 + 30^2}}{22} = 0.5253 \end{aligned}

Untransposed line

[L]=0.2[5.86321.06640.52531.06645.86321.06640.52531.06645.8632]=[1.17260.21330.10510.21331.17260.21330.10510.21331.1726] mH/km[L] = 0.2\begin{bmatrix} 5.8632 & 1.0664 & 0.5253 \\ 1.0664 & 5.8632 & 1.0664 \\ 0.5253 & 1.0664 & 5.8632 \end{bmatrix} = \begin{bmatrix} 1.1726 & 0.2133 & 0.1051 \\ 0.2133 & 1.1726 & 0.2133 \\ 0.1051 & 0.2133 & 1.1726 \end{bmatrix}\ \text{mH/km}

The mutual terms are not all equal (L12=L23≠L13L_{12} = L_{23} \ne L_{13}). So with balanced currents the voltage drops of the three phases are unequal, and the line is unbalanced.

Transposed line

Average the self and mutual terms:

Ls=0.2×5.8632=1.1726 mH/kmMm=1.0664+1.0664+0.52533=0.8860Lm=0.2×0.8860=0.1772 mH/km\begin{aligned} L_s &= 0.2 \times 5.8632 = 1.1726\ \text{mH/km} \\ M_m &= \frac{1.0664 + 1.0664 + 0.5253}{3} = 0.8860 \\ L_m &= 0.2 \times 0.8860 = 0.1772\ \text{mH/km} \end{aligned} [Lt]=[1.17260.17720.17720.17721.17260.17720.17720.17721.1726] mH/km[L_t] = \begin{bmatrix} 1.1726 & 0.1772 & 0.1772 \\ 0.1772 & 1.1726 & 0.1772 \\ 0.1772 & 0.1772 & 1.1726 \end{bmatrix}\ \text{mH/km}

Sequence inductances:

L1=L2=Ls−Lm=1.1726−0.1772=0.9954 mH/kmL0=Ls+2Lm=1.1726+0.3544=1.5271 mH/km\begin{aligned} L_1 = L_2 &= L_s - L_m = 1.1726 - 0.1772 = 0.9954\ \text{mH/km} \\ L_0 &= L_s + 2L_m = 1.1726 + 0.3544 = 1.5271\ \text{mH/km} \end{aligned}

Check with the GMD formula

Deq=11×11×223=13.86D_{eq} = \sqrt[3]{11 \times 11 \times 22} = 13.86 m, so

L1=0.2ln⁡13.860.08526=1.018 mH/kmL_1 = 0.2\ln\frac{13.86}{0.08526} = 1.018\ \text{mH/km}

This is close to 0.995 mH/km; the small difference is due to the effect of the ground images.

Answer: untransposed Lii=1.1726L_{ii} = 1.1726, L12=0.2133L_{12} = 0.2133, L13=0.1051L_{13} = 0.1051 mH/km; transposed Ls=1.1726L_s = 1.1726, Lm=0.1772L_m = 0.1772 mH/km, positive-sequence L1=0.995L_1 = 0.995 mH/km.

✓ Answer checked by Claude Opus 5.5 (high effort)

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