The emf induced in the second coil is given by:
\[ \text{EMF} = -M \frac{di}{dt} \]
Substitute \( i = i_0 \sin \omega t \):
\[ \frac{di}{dt} = i_0 \omega \cos \omega t \]
Thus, the maximum emf (when \( \cos \omega t = 1 \)) is:
\[ \text{EMF}_{\text{max}} = Mi_0 \omega = (0.002) \times (5) \times (50\pi) = \frac{\pi}{2} \, \text{V} \]
Therefore, \(\alpha = 2\).
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.}
Match List-I with List-II: List-I