Ferranti Effect: 3 Shocking Reasons Voltage Rises at No Load

Share:
Power Systems
Ferranti Effect: 3 Shocking Reasons Voltage Rises at No Load

On a long line with little load, the far end voltage can climb above the source, the opposite of what most people expect.

Line Charging Current Long Transmission Lines Shunt Reactors Voltage Rise

The Ferranti effect is the rise of receiving end voltage above sending end voltage on a long, lightly loaded line or cable. It is caused by line capacitance drawing charging current through the series inductance.

Hello everyone, today we are going to understand the Ferranti effect, why voltage can rise at the far end of a lightly loaded line, how to estimate it, and how utilities control it.
Ferranti effect

What Is the Ferranti Effect?

The Ferranti effect is a condition where the receiving end voltage of a long AC line becomes higher than the sending end voltage under light or no load. It was first observed by Sebastian de Ferranti in the 1880s on underground cables in London, and it follows from basic impedance and reactance behaviour.

Normally we expect voltage to fall along a line because of load current. At light load, however, the line itself behaves like a capacitor and draws leading current.

circuit of a transmission line with series inductance and shunt capacitance
Image credit: EEPower

That leading charging current flows through the inductive reactance of the line. The resulting voltage drop is in phase with the source voltage and actually adds to it.

EEPower notes the effect is strongest on long lines and especially on cables, whose capacitance is far higher than that of overhead lines.

3 Shocking Reasons the Voltage Rises

1
Line Charging Current
Shunt capacitance draws leading current even with no load connected.
2
Inductive Drop Adds in Phase
Leading current through series inductance raises voltage along the line.
3
Length Squared Growth
The rise grows roughly with the square of line length.

Reason 1 depends on capacitance between conductors and to earth, which is distributed along every metre of the line.

Reason 2 is about phase angles, covered in phase angle in AC circuits. A leading current through an inductor produces a voltage that adds to the source rather than subtracting.

Put together, these three reasons explain why engineers watch voltage closely during light load hours, holidays and night time. Grid operators often see their highest system voltages at these times, not at peak demand.

Voltage Rise Formula With Example

Vr ÷ Vs = 1 ÷ cos(β × ℓ), with β = ω × √(L × C)
Approximate rise ≈ ω² × L × C × ℓ² ÷ 2

Worked example, overhead line at 50 Hz:
L = 1 mH per km, C = 0.011 µF per km, ℓ = 300 km
β = 314 × √(1 × 10^(minus 3) × 1.1 × 10^(minus 8)) = 0.00104 rad per km
β × ℓ = 0.3125 rad, cos = 0.9516
Vr ≈ 1.051 × Vs, about 5 percent rise at no load

Doubling the length to 600 km raises the no load rise to roughly 22 percent. This is why very long lines always need compensation.

EEPower notes the theoretical limit is reached near one quarter wavelength, about 1500 km at 50 Hz, where voltage would rise without bound on a lossless line.

When the Ferranti Effect Appears

Light Load at NightLoad current falls sharply
Line Energized OpenRemote breaker still open
Long CablesHigh capacitance per km
Charging Current DominatesLeading current exceeds load current
Receiving Voltage RisesPossible overvoltage at far end

Energizing a long line from one end with the far end open is a classic case. Operators often close the far end breaker quickly or connect reactors first.

Long underground and submarine cables show the effect even at moderate lengths. Their high capacitance means large charging currents at every voltage level.

The same phenomenon links to reactive power flow, covered in active, reactive and apparent power. Lines at light load generate more reactive power than they absorb.

Methods to Control the Ferranti Effect

Shunt Reactors
Absorb charging current at line ends or substations.
SVC and STATCOM
Dynamic reactive power control.
Switching Sequence
Close both ends quickly when energizing.
Tap Changers
Lower transformer taps at light load.
Generator Excitation
Run generators in under excitation.
Limit Line Length
Add intermediate substations on long routes.

Shunt reactors are the most common remedy. EEPower suggests limiting uncompensated lines to about 600 to 700 km at 50 Hz, with reactors added beyond that.

Switching out capacitor banks at light load also helps, since they add to the leading current.

Ferranti Effect on Lines vs Cables

FeatureOverhead LineUnderground Cable
Capacitance per kmLowHigh, often 20 to 50 times higher
Length before significant riseHundreds of kmTens of km
Typical remedyShunt reactors at endsReactors at both ends or mid route
Charging currentModerateLarge

Cable projects therefore study reactive compensation early. Long HVAC cable links often need reactors on both sides.

The resulting voltage profile is checked in voltage swell and insulation coordination studies.

No Load Voltage Rise Calculator

Receiving End Voltage at No Load
Voltage ratio
Vr = 1.051 × Vs, rise 5.1 percent

This lossless model slightly overestimates the rise on real lines with resistance. It is ideal for quick screening.

Key Takeaways
  • Occurs at light or no load.
  • Caused by charging current through inductance.
  • Grows with the square of length.
  • Controlled with shunt reactors.
Risks if Ignored
  • Overvoltage at remote substations.
  • Stress on insulation and arresters.
  • Equipment tripping on high voltage.
  • Trouble energizing long cables.

Ferranti Effect Explained PDF

PDF
Ferranti Effect Explained
Short technical note on causes, calculation and mitigation of voltage rise

Voltage Rise Video Explanation

Ferranti Effect FAQ

What is the Ferranti effect?
A rise of receiving end voltage above sending end voltage on long lightly loaded lines.
What causes it?
Line charging current flowing through the series inductance.
Does it happen on short lines?
The effect is negligible on short lines.
Why are cables more affected?
They have much higher capacitance per km.
How is it controlled?
Mainly with shunt reactors, plus SVCs and switching practices.
Does it occur at full load?
No, load current normally masks it.
At what length does it become severe?
Hundreds of km for lines and tens of km for cables.

Related Articles

External References

What We Learn Today

  • Light load lets charging current dominate and raise far end voltage.
  • The rise grows roughly with the square of line length.
  • Shunt reactors and good switching practice keep voltage in limits.
I hope you like above blog. There is no cost associated in sharing the article in your social media. Thanks for reading!! Happy Learning!!

Leave a Reply

Your email address will not be published. Required fields are marked *