The figure shows a square loop $L$ of side $5\, cm$ which is connected to a network of resistances.
The whole setup is moving towards right with a constant speed of $1\, cms^{-1}$. At some instant, a part of $L$ is in a uniform magnetic field of $1T$, perpendicular to the plane of the loop. If the resistance of $L$ is $1.7\, \Omega$ , the current in the loop at that instant will be close to :
Since it is a balanced wheatstone bridge, its equivalent resistance $ = \frac{4}{3} \Omega$$ \varepsilon = B \ell v = 5 \times 10^{-4} V$
So total resistance
$R = \frac{4}{3} + 1.7 \approx 3\Omega $$ \therefore \; i \frac{\varepsilon}{R} \approx 166 \mu A \; \approx \; 170 \mu A $
Electromagnetic Induction is a current produced by the voltage production due to a changing magnetic field. This happens in one of the two conditions:-
When we place the conductor in a changing magnetic field.
When the conductor constantly moves in a stationary field.