In the above figure
N and S are poles of a magnet, θ is the angle between the directions of magnetic field B and area vector A.
When the coil is rotated in the magnetic field, the flux linked with the coil varies. At any’ instant of time ‘t’, A cosθ is the component of area vector along the direction B.
The magnetic flux linked with the coil at any instant of time ‘t’ is given by
ΦB = B x component of area vector along the field direction.
For 1 turn ΦB = BA cos θ
For n turns ΦB = nAB cos θ
ΦB = nABcosωt….(1) [∵ θ = ωt]
Where ‘ω’ is the angular velocity of the coil at time t. From the Faraday’s second law,
e = \(\frac{\mathrm{d} \phi}{\mathrm{d} \mathrm{t}}\)
e = -\(\frac{\mathrm{d}}{\mathrm{dt}}\) [nAB cos cot]
[From (l) Φ = nABcosωt]
e = (-n AB) [-sin ωt) × ω
e = nABωsinωt
e = e0 sin(ωt)
where e0 is the peak value of emf = nAB ω