A thin copper ring of radius R=5.0cm and resistance r=2.0mΩ is placed horizontally above a solenoid coil. The solenoid has N=800 turns wound over a length L=20cm and radius a=3.0cm. When an alternating current I(t)=I0cos(ωt) with amplitude I0=15A and frequency f=60Hz flows through the solenoid, the ring experiences a time-averaged upward magnetic force that can balance its weight.
The ring has mass m=12g and is positioned at height h above the top of the solenoid, where the magnetic field from the solenoid can be approximated as that of a magnetic dipole: Bz(z)=2πz3μ0M along the axis, where M=21πa2NI(t) is the magnetic dipole moment and z is the distance from the solenoid center.
(a) Find the time-averaged power dissipated in the ring when it is at equilibrium height h.
(b) Determine the equilibrium height h where the ring levitates.
Take μ0=4π×10−7H/m and g=9.8m/s2.