The Levitating Ring · AI Generator #GEN-B463752F

Physics · electromagnetism

Problem

A research team is studying magnetic levitation using a unique setup. A thin conducting ring of radius R=5.0  cmR = 5.0\;\text{cm} and resistance r=0.20  Ωr = 0.20\;\text{Ω} is placed horizontally above a solenoid coil. The solenoid has N=500N = 500 turns wound tightly over a length L=8.0  cmL = 8.0\;\text{cm} and radius a=3.0  cma = 3.0\;\text{cm}. The solenoid carries a current I(t)=I0sin⁡(ωt)I(t) = I_0 \sin(\omega t) where I0=12  AI_0 = 12\;\text{A} and ω=2π×60  Hz\omega = 2\pi \times 60\;\text{Hz}. When the ring is positioned at height h=6.0  cmh = 6.0\;\text{cm} 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)=μ0NI2L(a2a2+h2)B(h) = \frac{\mu_0 N I}{2L}\left(\frac{a^2}{a^2 + h^2}\right) 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×10−7  H/m\mu_0 = 4\pi \times 10^{-7}\;\text{H/m}.

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