Let G be the resistance of the galvanometer and ig the current, which on passing through the galvanometer, produces full-scale deflection.
Suppose V is the maximum potential difference to be measured which exists between points a and b. On connecting the galvanometer across a and b a current ig flows through it. Then from Ohm's law we have. ig=G+RV G+R=igV ⇒R=igV−G
Thus, on connecting a resistance R of above value in series with the galvanometer the galvanometer will become a voltmeter of range 0 to V volts.
The value of resistance should be high enough so that it does not draw any current from the circuit.
Resistance of an ideal voltmeter is high.