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In measuring resistance by voltmeter-ammeter method, the voltmeter can be connected either across supply or across the resistance. If the resistance is low, the voltmeter should be connected
1. across the supply
2. across the resistance
3. either across the supply or across the resistance
4. neither across the supply nor across the resistance

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Correct Answer - Option 2 : across the resistance

V–A Method:

In this method, the voltmeter is connected across the supply.

V = Voltmeter reading

A = Ammeter reading

VL = Voltage across load R.

IL = Current flowing through load R.

R = Unknown resistance to be measured

Ra = Internal resistance of the ammeter

Va= voltage drop across ammeter.

V = VL + Va

\({R_{meas}} = \frac{V}{A} = \frac{V}{{{I_L}}} = \frac{{{V_L} + {V_a}}}{{{I_L}}}\)

but \({R_{true}} = \frac{{{V_L}}}{{{I_L}}} = R\)

Rmeas = Rtrue + Ra

So, in this method measured value is greater than the true value. This error is due to an ammeter.

Error \( = \frac{{{R_{meas}} - {R_{true}}}}{{{R_{true}}}} = \frac{{{R_a}}}{R}\)

The error is high for very low values of unknown resistance R.

A–V Method:

In this method, the voltmeter is connected across the resistance.

V = Voltmeter reading

A = Ammeter reading

VL = Voltage across load R.

R = Unknown resistance to be measured

IL = Current flowing through load R.

IV = Current flowing through the voltmeter.

\({R_{meas}} = \frac{{{V_L}}}{{\left( {{I_L} + {I_V}} \right)}} = \frac{V}{{\frac{V}{R} + \frac{V}{{{R_V}}}}} = \frac{{R{R_V}}}{{R + {R_V}}}\)

\({R_{true}} = \frac{{{V_L}}}{{{I_L}}} = R\)

The measured value is less than the true value. In this method, the error is due to the voltmeter.

Error \( = \frac{{{R_{meas}} - {R_{true}}}}{{{R_{true}}}} = - \frac{R}{{{R_V}}}\)

The error is low for very low values of unknown resistance R.

Observations:

  • In both methods errors due to load side instruments.
  • V – A method is best suitable for high resistances in the medium range.
  • A – V method is best suitable for low resistances in the medium range.

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