Answer:
fem = -A β
Explanation:
Faraday's law gives the induced electromotive source (emf)
fem = [tex]- \ \frac{d \phi_B }{dt}[/tex]
the magnetic flux is
[tex]\phi_B[/tex] = B. A = B A cos θ
the bold are vectros. In this case the normal to the ring is parallel to the magnetic field so the angle is zero cos 0 = 1, also the area of the ring is constant
fem = -A [tex]\frac{dB}{dt}[/tex]
we carry out the derivative of the function B = α + β t
fem = -A β
so we see that there is an electromotive force in the ring.