Initially,a rectangular coil with its length vertical is moving out with a constant velocity $v$ in a constant magnetic field $B$ towards the right. Now,the same coil is rotated through $90^{\circ}$ in the same plane in the same magnetic field $B$,and the coil is moving with the same velocity $v$. The magnitude of the induced e.m.f. is now

  • A
    greater than the initial induced e.m.f.
  • B
    less than the initial induced e.m.f.
  • C
    equal to the initial induced e.m.f.
  • D
    sometimes greater and sometimes less than the initial induced e.m.f.

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$A$ wheel with radial metal spokes $1 \ m$ in length is rotated in a magnetic field of $0.5 \times 10^{-4} \ T$ normal to the plane of the wheel. If the induced emf between the rim and axle is $\pi / 3000 \ V$,then the rotational speed of the wheel in revolutions per minute is

$A$ conducting rod of length $\ell$ moves with a velocity $V$ in a uniform magnetic field $B$ perpendicular to the plane of the rails. $A$ capacitor of capacitance $C$ is connected across the rails as shown. Find the charge on the capacitor due to the induced emf in the rod.

An equilateral triangular loop $ADC$ moves out of a finite magnetic field $B$ as shown in the figure. At time $t = 0$, side $DC$ of the loop is at the edge of the magnetic field. The magnetic field is perpendicular to the paper inwards (or perpendicular to the plane of the coil). The induced current versus time graph will be as:

$A$ conducting wire is moving towards the right in a magnetic field $B$. The direction of the induced current $i$ in the wire is shown in the figure. The direction of the magnetic field will be

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