Let’s use the Faraday’s law and find the induced emf in the coil:
E=-(dΦ_B)/dt,
here, E is the emf generated between the ends of the coil, Φ_B=NBAcosθ=NBAcos0^°=NBA is the magnetic flux through the coil, N is the number of turns of the coil, B is the magnetic field, A=πr^2 is the cross-sectional area of the coil, r is the radius of the circular coil, θ is the angle between the magnetic field and the normal to the plane of the coil (since the magnetic field directed perpendicularly to the plane of the coil, θ=0^°).
Then, we get:
E=-(dΦ_B)/dt=-d(NBA)/dt=-NA dB/dt=-Nπr^2 d/dt (0.01t+0.04t^2 )==-Nπr^2 (0.01+0.08t),
E(t=5 s)=-30∙π(0.04 m)^2 (0.01+0.08∙5 s)=-0.0618 V=-61.8 mV.
Answer:
E(t=5 s)=-61.8 mV.
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