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The voltmeter is ideal so it doesn't draw any current from the circuit.
Potential difference across resistance = (given)
So the current in the resistance =
i.e.,
The same current passes through . The resistors and are in series and their equivalent, i.e., is in parallel with between and . Dividing the current in the inverse ratio of resistances between and ,
and
at junction divides into three parts. Since the resistances are in parallel between and , current will distribute in the inverse ratio of resistances.
So
( being a constant of proportionality)
and
but
or
so
Thus current through resistance is
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