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, \(\alpha = 2\).
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