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ElectricalMeasurement & Instrumentation
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A repulsion type ammeter when used on A.C circuit reads

A

Peak value of current

B

R.M.S value of the current

C

Mean value of current

D

Equivalent D.C value of the current

Correct Answer

Concept & PrincipleElectricalMeasurement & Instrumentation
Option B

R.M.S value of the current

Quick Summary: A repulsion-type moving iron ammeter operates on the principle of magnetic repulsion between two soft-iron vanes placed within a current-carrying coil. Because the deflecting torque is proportional to the square of the current ($T_d \propto I^2$), the instrument responds to the mean square of the instantaneous current, thereby measuring the Root Mean Square (R.M.S.) value regardless of the current's waveform.

ЁЯТб Explanation

A repulsion-type moving iron ammeter operates on the principle of magnetic repulsion between two soft-iron vanes placed within a current-carrying coil. Because the deflecting torque is proportional to the square of the current (TdтИЭI2T_d \propto I^2TdтАЛтИЭI2), the instrument responds to the mean square of the instantaneous current, thereby measuring the Root Mean Square (R.M.S.) value regardless of the current's waveform.

ЁЯФв Key Formulas

Td=I2dMd╬╕T_d = I^2 \frac{dM}{d\theta}TdтАЛ=I2d╬╕dMтАЛ тАФ Deflecting torque for moving iron instruments

Irms=1TтИл0Ti(t)2dtI_{rms} = \sqrt{\frac{1}{T} \int_{0}^{T} i(t)^2 dt}IrmsтАЛ=T1тАЛтИл0TтАЛi(t)2dtтАЛ тАФ Definition of R.M.S value

тЪЩя╕П Working Principle

When current passes through the fixed coil, it magnetizes both the fixed and moving iron vanes in the same polarity. This creates a repulsive force proportional to the product of the pole strengths, which are both proportional to the instantaneous current iii. Thus, the instantaneous torque is Ti=kтЛЕi2T_i = k \cdot i^2TiтАЛ=kтЛЕi2. The inertia of the moving system causes it to respond to the average torque, which is Tavg=kтЛЕ1TтИл0Ti2dt=kтЛЕIrms2T_{avg} = k \cdot \frac{1}{T} \int_{0}^{T} i^2 dt = k \cdot I_{rms}^2TavgтАЛ=kтЛЕT1тАЛтИл0TтАЛi2dt=kтЛЕIrms2тАЛ.

ЁЯУМ Key Points
  • тЦ╕

    Moving iron instruments are inherently R.M.S responding.

  • тЦ╕

    They can be used for both A.C. and D.C. measurements.

  • тЦ╕

    The scale of a repulsion type ammeter is non-uniform (cramped at the beginning).

  • тЦ╕

    It is unaffected by the waveform of the alternating current.

тЬЕ Advantages
  • тЦ╕

    Low cost and robust construction

  • тЦ╕

    Can measure both A.C. and D.C. currents

тЭМ Disadvantages / Limitations
  • тЦ╕

    Non-linear (cramped) scale

  • тЦ╕

    Errors due to hysteresis and frequency variations

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Industrial power frequency ammeters

  • тЦ╕

    Low-cost laboratory measurement devices

ЁЯУД Additional Information
  • тЦ╕

    The repulsion type is specifically used for ammeters and voltmeters.

  • тЦ╕

    Option A (Peak value) is measured by Peak-reading voltmeters. Option C (Mean value) is measured by Rectifier-type instruments calibrated to read the R.M.S of a sine wave.

ЁЯУК Diagram / Illustration
Moving Iron Meter Principle
TdтИЭIrms2T_d \propto I_{rms}^2TdтАЛтИЭIrms2тАЛ
Result: Reads R.M.S value
тЬЕ

B is correct тАФ Repulsion type moving iron instruments measure the R.M.S value of current because their deflection is proportional to the square of the current.

Core Concepts Used
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Moving Iron Instrument R.M.S Value Electromagnetic Repulsion
ЁЯТб EXAM TIP

Always remember that moving iron (MI) meters read R.M.S, whereas moving coil (PMMC) meters read the average (mean) value of the current.

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