A plane circular coil is rotated about its vertical diameter with a constant angular speed \(\omega\) in a uniform horizontal magnetic field. Initially the plane of the coil is parallel to the magnetic field. Draw the plot showing the variation of induced emf \(e\) in the coil as a function of \(\omega t\), where \(t\) represents the time elapsed.
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Whenever
\[
\phi=\phi_0\sin(\omega t),
\]
Faraday's law gives
\[
e=-\frac{d\phi}{dt}
=-e_0\cos(\omega t).
\]
Thus, the induced emf leads or lags the flux by \(90^\circ\) depending upon the chosen sign convention.