Step 1: Understanding the Concept
The flux through the loop is \(\phi=Ba^{2}\cos\theta\) with \(\theta=\omega t\), the angle between \(\vec{B}\) and the normal.
Step 2: Induced emf
\(e=-\dfrac{d\phi}{dt}=Ba^{2}\omega\sin\omega t\).
Step 3: Maximum value
The emf is largest when \(\sin\theta=1\), that is, first at \(\theta=90^{\circ}\). There the loop plane is parallel to the field and the flux is zero but changing fastest.
So \(e_{max}=Ba^{2}\omega\).
Final Answer:
The maximum emf is \(Ba^{2}\omega\), first at \(\theta=90^{\circ}\).
\[ \boxed{\text{(A) }Ba^{2}\omega ;\ \theta =90^{\circ }} \]