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: \( \text{(A) 22 V} \)
Conductor wire ABCDE with each arm 10 cm in length is placed in magnetic field of $\frac{1}{\sqrt{2}}$ Tesla, perpendicular to its plane. When conductor is pulled towards right with constant velocity of $10 \mathrm{~cm} / \mathrm{s}$, induced emf between points A and E is _______ mV.}
Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: