Step 1: Initial condition.
The plane of the coil is initially parallel to the magnetic field.
Hence, angle between area vector and field: \( \theta = 90^\circ \)
\[
\phi = 0 \text{ at } t = 0
\]
Step 2: Magnetic flux as coil rotates.
For a coil rotating with angular speed \( \omega \):
\[
\theta = \omega t + \frac{\pi}{2}
\]
\[
\phi = BA \cos\left(\omega t + \frac{\pi}{2}\right) = BA \sin(\omega t)
\]
Graph:
Magnetic flux \( \phi \) varies sinusoidally with time, starting from zero.
Hence, \( \phi \) vs \( \omega t \) is a sine curve starting at the origin.
Step 3: Induced emf.
\[
e = -\frac{d\phi}{dt} = -BA\omega \cos(\omega t)
\]
Graph:
The induced emf \( e \) follows a cosine curve:
- Maximum at \( t = 0 \)
- Phase difference of \( 90^\circ \) with flux
Step 4: Graph Summary.
(a) \( \phi \) vs \( \omega t \): sine wave starting from zero
(b) \( e \) vs \( \omega t \): cosine wave starting from maximum value