The emf induced in a coil is given by Faraday's law of electromagnetic induction: \[ \mathcal{E} = -\frac{d\phi}{dt} \] where:
- \( \mathcal{E} \) is the induced emf,
- \( \phi \) is the magnetic flux. The magnetic flux is given by: \[ \phi = (4t^2 + 6t + 9) \, \text{Wb} \] To find the induced emf, we differentiate \( \phi \) with respect to \( t \): \[ \frac{d\phi}{dt} = \frac{d}{dt} \left( 4t^2 + 6t + 9 \right) \] Differentiating term by term: \[ \frac{d\phi}{dt} = 8t + 6 \] Now, substituting \( t = 2 \) seconds into the equation: \[ \frac{d\phi}{dt} = 8(2) + 6 = 16 + 6 = 22 \, \text{V} \]
Therefore, the induced emf at \( t = 2 \) seconds is: \[ \mathcal{E} = 22 \, \text{V} \]
Thus, the correct answer is: \( \text{(A) 22 V} \)
Show that the energy required to build up the current \( I \) in a coil of inductance \( L \) is \( \frac{1}{2} L I^2 \).
A circular coil of diameter 15 mm having 300 turns is placed in a magnetic field of 30 mT such that the plane of the coil is perpendicular to the direction of the magnetic field. The magnetic field is reduced uniformly to zero in 20 ms and again increased uniformly to 30 mT in 40 ms. If the EMFs induced in the two time intervals are \( e_1 \) and \( e_2 \) respectively, then the value of \( e_1 / e_2 \) is:
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: