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.