A research team is studying magnetic levitation using a unique setup. A thin conducting ring of radius R=5.0cm and resistance r=0.20Ω is placed horizontally above a solenoid coil. The solenoid has N=500 turns wound tightly over a length L=8.0cm and radius a=3.0cm. The solenoid carries a current I(t)=I0sin(ωt) where I0=12A and ω=2π×60Hz.
When the ring is positioned at height h=6.0cm above the top of the solenoid, the magnetic field at the ring's location due to the solenoid is approximately uniform across the ring's area and has magnitude:
B(h)=2Lμ0NI(a2+h2a2)
Due to the time-varying current, an EMF is induced in the ring, causing a current to flow. This current interacts with the magnetic field to produce a force on the ring.
(a) Find the magnitude of the induced EMF in the ring as a function of time.
(b) Calculate the time-averaged power dissipated in the ring over one complete cycle.
(c) Determine the maximum instantaneous upward magnetic force on the ring. Use μ0=4π×10−7H/m.