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: \( \text{(A) 22 V} \)
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: