Skip to main content

Inductance and capacitance of 4-conductor bundle line

Short answer

Mutual GMD = 7.5595 m. Inductance: bundle GMR using r'=0.009346 m is 0.18629 m, L = 2e-7 ln(7.5595/0.18629)=0.7407 mH/km. Capacitance: bundle GMR using r=0.012 m is0.19830 m, C = 2*pi*epsilon0/ln(7.5595/0.19830)=15.28 nF/km. For 200 km, L=148.1 mH, C=3.056 µF.

A 220 kV, 50 Hz, 200 km long 3-phase line has conductors spaced as shown in the figure below. Compute the inductance and capacitance per phase. Each sub-conductor is of 12 mm radius. Assume transposed configuration of the line. [Figure: horizontal single-circuit line; each phase A, B, C is a square bundle of four sub-conductors (1,2,3,4) with 45 cm sides; centres of adjacent phases 6 m apart.]

Each phase is a 4-conductor square bundle, so we find the bundle GMR (self-GMD) and the mutual GMD between phase centres, then use the standard formulas for a transposed line.

   o o        o o        o o
   o o        o o        o o
    A    6 m   B    6 m   C
   |<------- 12 m ------->|
 square side d = 0.45 m, r = 12 mm

Data: r=0.012r = 0.012 m, d=0.45d = 0.45 m, DAB=DBC=6D_{AB} = D_{BC} = 6 m, DCA=12D_{CA} = 12 m, length 200 km.

Mutual GMD

Dm=6×6×123=7.5595 mD_m = \sqrt[3]{6 \times 6 \times 12} = 7.5595\ \text{m}

Self GMD of a 4-conductor bundle

For a square bundle, Ds=(rx⋅d⋅d⋅2d)1/4=1.09 (rxd3)1/4D_s = (r_x \cdot d \cdot d \cdot \sqrt{2}d)^{1/4} = 1.09\,(r_x d^3)^{1/4}.

  • Inductance: r′=0.7788×0.012=0.009346r' = 0.7788 \times 0.012 = 0.009346 m
DsL=1.09 (0.009346×0.453)1/4=0.18629 mD_{sL} = 1.09\,(0.009346 \times 0.45^3)^{1/4} = 0.18629\ \text{m}
  • Capacitance (uses actual radius rr):
DsC=1.09 (0.012×0.453)1/4=0.19830 mD_{sC} = 1.09\,(0.012 \times 0.45^3)^{1/4} = 0.19830\ \text{m}

Inductance per phase

L=2×10−7ln⁡DmDsL=2×10−7ln⁡7.55950.18629=2×10−7×3.7033=7.4065×10−7 H/m=0.7407 mH/km\begin{aligned} L &= 2\times10^{-7}\ln\frac{D_m}{D_{sL}} = 2\times10^{-7}\ln\frac{7.5595}{0.18629} \\ &= 2\times10^{-7}\times 3.7033 = 7.4065\times10^{-7}\ \text{H/m} \\ &= 0.7407\ \text{mH/km} \end{aligned}

For 200 km: L=0.7407×200=148.13L = 0.7407 \times 200 = 148.13 mH.

Capacitance per phase (to neutral)

C=2πε0ln⁡(Dm/DsC)=2π×8.854×10−12ln⁡(7.5595/0.19830)=55.63×10−123.6408=15.28×10−12 F/m=15.28 nF/km\begin{aligned} C &= \frac{2\pi\varepsilon_0}{\ln(D_m/D_{sC})} = \frac{2\pi \times 8.854\times10^{-12}}{\ln(7.5595/0.19830)} \\ &= \frac{55.63\times10^{-12}}{3.6408} = 15.28\times10^{-12}\ \text{F/m} \\ &= 15.28\ \text{nF/km} \end{aligned}

For 200 km: C=15.28×200=3056C = 15.28 \times 200 = 3056 nF =3.056 μ= 3.056\ \muF.

Answer: L=0.7407L = 0.7407 mH/km per phase (148.13 mH for 200 km); C=15.28C = 15.28 nF/km per phase to neutral (3.056 µF for 200 km).

✓ Answer checked by Claude Opus 5.5 (high effort)

All Power System Analysis I chapter 4 questions →