A conducting square loop initially lies in the XZ plane with its lower edge hinged along the X-axis. Only in the region \( y \ge 0 \), there is a time dependent magnetic field pointing along the Z-direction, \( \vec{B}(t)=B_{0}(\cos \omega t)\,\hat{k} \), where \( B_{0} \) is a constant. The magnetic field is zero everywhere else. At time \( t=0 \), the loop starts rotating with constant angular speed \( \omega \) about the X axis in the clockwise direction as viewed from the \( +X \) axis (as shown in the figure). Ignoring self-inductance of the loop and gravity, which of the following plots correctly represents the induced e.m.f. (\( V \)) in the loop as a function of time:
