(d) Whenever a magnet is moved either towards or away from a conducting coil, the magnetic flux linked with the coil changes and therefore, an emf is induced in the coil. The magnitude of induced emf
$\ \ \ \ \ \ \ \ \ e = - N\ \frac{d\phi}{dt}$
$\ \ \ \ \ \ \ \ e = - N\ \frac{d(BA)}{dt}$
Time interval$\ dt$, depends on the speed with which the magnet is moved.
Therefore, the induced emf is independent of the resistance of the coil.