The magnetic flux \( \phi \) is given by:
\[
\phi = B \cdot A = AB
\]
At the instant when \( B \) is parallel to the plane of the coil, the induced emf \( \varepsilon \) is given by:
\[
\varepsilon = -N \frac{d\phi}{dt}
\]
Since \( \phi = AB \), and the coil is rotating with angular velocity \( \omega \), we have:
\[
\varepsilon = -N \frac{d(AB)}{dt} = -N \cdot A \cdot B \cdot \omega = NAB\omega
\]