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220 kV double circuit efficiency and regulation

Short answer

Using nominal-π model, two parallel circuits, 0.9 pf lag: efficiency is98.93%, voltage regulation2.57%, no-load receiving-end voltage225.65 kV (5.65 kV rise above rated). The line already exceeds the94% efficiency and12% regulation limits; if needed, larger conductors, shunt capacitors, or series compensation could further improve performance.

A double circuit, 220 kV, 50 Hz, three phase transmission line is designed to carry 144 MW for 130 km. The line constants are given as: R = 0.0544 Ω/km (at max allowable temp.), L = 0.494 mH/km, C = 23.1 nF/km. Calculate the following: a) Transmission line efficiency b) Percentage of voltage regulation c) Value of receiving end voltage rise at no load if sending end voltage is held constant. Suggest the options to get efficiency > 94% and voltage regulation < 12%.

The line is 130 km long, so it is a medium line and the nominal-π model is used. The two circuits are in parallel.

Assumptions: power factor 0.9 lagging (not given in the question); receiving-end voltage held at 220 kV.

Line parameters (per phase)

Per circuit:

R=0.0544×130=7.072 ΩX=2π(50)(0.494×10−3)(130)=20.175 ΩY=2π(50)(23.1×10−9)(130)=9.434×10−4 S\begin{aligned} R &= 0.0544 \times 130 = 7.072\ \Omega \\ X &= 2\pi(50)(0.494\times10^{-3})(130) = 20.175\ \Omega \\ Y &= 2\pi(50)(23.1\times10^{-9})(130) = 9.434\times10^{-4}\ \text{S} \end{aligned}

Two circuits in parallel:

Z=7.072+j20.1752=3.536+j10.088 Ω,Y=j1.887×10−3 SZ = \frac{7.072 + j20.175}{2} = 3.536 + j10.088\ \Omega, \qquad Y = j1.887\times10^{-3}\ \text{S}

Constants and currents

A=1+ZY2=0.9905∠0.19°VR=2203=127.02∠0° kVIR=144×1063×220×103×0.9=419.9∠−25.84° A\begin{aligned} A &= 1 + \frac{ZY}{2} = 0.9905\angle 0.19° \\ V_R &= \frac{220}{\sqrt{3}} = 127.02\angle 0°\ \text{kV} \\ I_R &= \frac{144\times10^6}{\sqrt{3}\times220\times10^3\times0.9} = 419.9\angle -25.84°\ \text{A} \end{aligned} VS=AVR+ZIR=129.04∠1.59° kV/phase=223.51 kV (line)IS=CVR+AIR=379.1∠8.88° A\begin{aligned} V_S &= AV_R + ZI_R = 129.04\angle 1.59°\ \text{kV/phase} \\ &= 223.51\ \text{kV (line)} \\ I_S &= CV_R + AI_R = 379.1\angle 8.88°\ \text{A} \end{aligned}

a) Efficiency

PS=Re(3VSIS∗)=145.56 MWLoss=1.56 MWη=144145.56×100=98.93%\begin{aligned} P_S &= \text{Re}(3V_SI_S^*) = 145.56\ \text{MW} \\ \text{Loss} &= 1.56\ \text{MW} \\ \eta &= \frac{144}{145.56}\times100 = 98.93\% \end{aligned}

b) Voltage regulation

At no load, VR0=VS/∣A∣V_{R0} = V_S/|A|:

VR0=223.510.9905=225.65 kV (line)%VR=225.65−220220×100=2.57%\begin{aligned} V_{R0} &= \frac{223.51}{0.9905} = 225.65\ \text{kV (line)} \\ \%VR &= \frac{225.65 - 220}{220}\times100 = 2.57\% \end{aligned}

c) Receiving-end voltage rise at no load (Ferranti effect)

With VSV_S held at 223.51 kV and the load removed:

ΔV=VR0−VS=225.65−223.51=2.15 kV\Delta V = V_{R0} - V_S = 225.65 - 223.51 = 2.15\ \text{kV}

The no-load voltage is 5.65 kV above the rated 220 kV.

Answer: η = 98.93%, VR = 2.57%, no-load rise = 2.15 kV above VSV_S (receiving end 225.65 kV).

The line already meets η > 94% and VR < 12% by a wide margin.

Options if the limits were not met

  1. Larger conductor (lower RR) for higher efficiency, or bundled conductors (lower XX) for better regulation.
  2. Raise the power factor with shunt capacitors or SVCs at the load end. At unity pf the regulation falls to about 1.1%.
  3. Series capacitor compensation to cut XX and the voltage drop.
  4. More circuits or a higher voltage (for example 400 kV), which reduces the current and therefore I2RI^2R and IXIX.
  5. Shunt reactors at the receiving end to limit the no-load (Ferranti) rise.
  6. On-load tap-changing transformers to correct the receiving-end voltage.

✓ Answer checked by Claude Opus 5.5 (high effort)

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