We use the integral form of Faraday's Law,
$\begin{align*}\int_P \mathbf{E} \cdot d \mathbf{l} = -\frac{d }{dt} \left(\int_S \mathbf{B} \cdot d \mathbf{a} \right) = \fra...$
If we take the path $P$ to be the circular wire loop (and we neglect the fact that it appears not to be a complete circle in the figure), then the left-hand side of the equation above is equal to the induced emf.
$\begin{align*}\phi_B = \pi R^2 B \cos \theta \end{align*}$
where $\theta$ is the angle between the normal to the circular loop and the magnetic field. The wire loop rotates with an angular speed of $\omega$ , therefore, $\theta = \omega t + \delta$ where $\delta$ is a constant.
$\begin{align*}\left|\frac{d \phi_B}{dt} \right| = \left|\varepsilon\right| = \varepsilon_0 \sin \omega t\end{align*}$
$\begin{align*}\frac{d \phi_B}{dt} = - \omega \pi R^2 B \sin \left(\omega t + \delta \right)\end{align*}$
So,
$\begin{align*}\left|\omega \pi R^2 B \sin \left(\omega t + \delta \right) \right| = \left| \varepsilon_0 \sin \omega t \right...$
This equation can only hold if
$\begin{align*}\left| \sin \left(\omega t + \delta \right) \right| = \left| \sin \omega t \right|\end{align*}$
It follows then that
$\begin{align*}\omega = \frac{\varepsilon_0}{\pi R^2 B}\end{align*}$
Therefore, answer (C) is correct.

Solution to 1996 Problem 46