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HV AC measurement methods and electrostatic voltmeter

Short answer

Methods: series impedance ammeter, potential dividers (resistive/capacitive), potential transformers, electrostatic voltmeters, peak voltmeters (Chubb-Fortescue), sphere gap. An electrostatic voltmeter uses the force between charged plates (F ∝ V²) to read true rms. In the attracted-disc type, a movable disc inside a guard ring is deflected; deflection measured via spring and mirror scale.

What are the different methods for measurement of high AC voltages? With neat diagram, explain the working principle of electrostatic voltmeter.

Methods for measurement of high AC voltages

MethodWhat it readsRemarks
Series impedance ammeter (R or C in series with ammeter)rms or meanSimple; errors from stray capacitance and harmonics
Potential dividers (resistive, capacitive, mixed) with LV meterrms / peakCapacitive dividers common for AC
Potential transformers (electromagnetic, CVT)rmsUsed up to a few hundred kV
Electrostatic voltmetertrue rmsNegligible loading
Peak voltmeters (Chubb–Fortescue, capacitor-rectifier)peakPeak decides breakdown
Sphere gappeakStandard calibrating device, ±3%

Electrostatic voltmeter

An electrostatic voltmeter measures voltage from the attractive force between two charged electrodes. Since the force depends on V2V^2, it reads the true rms value of AC (of any waveform) and the value of DC, and it draws almost no current.

Principle

For two parallel plates of area AA separated by xx, the stored energy is W=12CV2W = \frac12 CV^2 with C=ε0A/xC = \varepsilon_0 A/x. The force between the plates is

F=dWdx=12V2dCdx=−12 ε0AV2x2(attraction)\begin{aligned} F &= \frac{dW}{dx} = \frac12 V^2\frac{dC}{dx} \\ &= -\frac12\,\frac{\varepsilon_0 A V^2}{x^2}\quad(\text{attraction}) \end{aligned}

For AC, V=Vmsin⁡ωtV = V_m\sin\omega t, and the moving system responds to the average force:

Fav=ε0A2x2⋅1T∫0Tv2 dt=ε0A2x2Vrms2F_{av} = \frac{\varepsilon_0 A}{2x^2}\cdot\frac1T\int_0^T v^2\,dt = \frac{\varepsilon_0 A}{2x^2}V_{rms}^2

So the deflection measures VrmsV_{rms}.

Construction (attracted-disc type)

          HV electrode  (V)
   ===============================
                 |  gap x
   ======  [ movable disc ]  =====
   guard     |  (earthed)    guard
   ring      |               ring
             +-- spring / balance
             +-- mirror -> lamp & scale
                 |
               earth
  • High-voltage electrode: a large plane disc (or sphere) connected to the voltage to be measured.
  • Low-voltage electrode: an earthed plane with a guard ring; a small movable disc sits in a hole at its centre, flush with the plane.
  • The guard ring keeps the field over the movable disc uniform, so the simple parallel-plate formula holds and edge effects are removed.
  • The movable disc is held by a spring or a balance beam. Its small movement is magnified by a mirror and light beam on a scale, or the force is balanced by weights or a restoring spring (absolute instruments such as the Kelvin attracted-disc electrometer).
  • The whole system may be enclosed in compressed gas (N₂, SF₆) or vacuum to raise the range.

Working

  1. Voltage is applied between the HV electrode and the earthed plane.
  2. The movable disc is attracted towards the HV electrode with force proportional to V2V^2.
  3. The disc moves until the spring force balances the electrostatic force; the deflection is read on the scale, calibrated directly in kV.
  4. For range change, the gap xx is adjusted (larger gap for higher voltage).

Features

AdvantagesLimitations
Reads true rms of any waveformForce is small; needs careful calibration
Very small loading (a few pF)Not suitable for impulse voltages
Works on DC and AC up to about 1 MHzAffected by dust, external fields
Accuracy about ±0.1% to ±1%Bulky for very high voltages
No power drawn after chargingSquare-law scale (cramped at low end)

Ranges of about 600 kV in air and up to about 1000 kV with compressed gas insulation are achieved.

✓ Answer checked by Claude Opus 5.5 (high effort)

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