The Levitating Ring · AI Generator #GEN-F969C165

Physics · electromagnetism

Problem

A thin copper ring of radius R=5.0  cmR = 5.0\;\text{cm} and resistance r=2.0  mΩr = 2.0\;\text{m}\Omega is placed horizontally above a solenoid coil. The solenoid has N=800N = 800 turns wound over a length L=20  cmL = 20\;\text{cm} and radius a=3.0  cma = 3.0\;\text{cm}. When an alternating current I(t)=I0cos⁡(ωt)I(t) = I_0 \cos(\omega t) with amplitude I0=15  AI_0 = 15\;\text{A} and frequency f=60  Hzf = 60\;\text{Hz} flows through the solenoid, the ring experiences a time-averaged upward magnetic force that can balance its weight. The ring has mass m=12  gm = 12\;\text{g} and is positioned at height hh above the top of the solenoid, where the magnetic field from the solenoid can be approximated as that of a magnetic dipole: Bz(z)=μ0M2πz3B_z(z) = \frac{\mu_0 M}{2\pi z^3} along the axis, where M=12πa2NI(t)M = \frac{1}{2}\pi a^2 N I(t) is the magnetic dipole moment and zz is the distance from the solenoid center. (a) Find the time-averaged power dissipated in the ring when it is at equilibrium height hh. (b) Determine the equilibrium height hh where the ring levitates. Take μ0=4π×10−7  H/m\mu_0 = 4\pi \times 10^{-7}\;\text{H/m} and g=9.8  m/s2g = 9.8\;\text{m/s}^2.

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