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JEE Advanced 2023 Paper 2 · Physics · Electromagnetic Induction and Alternating Current · hard

A thin uniform metal disc of radius a=0.50 m can rotate without friction about its geometric axis, which is parallel to a uniform magnetic field…

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A thin uniform metal disc of radius a=0.50 ma=0.50\ \mathrm{m} can rotate without friction about its geometric axis, which is parallel to a uniform magnetic field B=2.0 TB=2.0\ \mathrm{T} perpendicular to the plane of the disc. A resistor R=1.0 ΩR=1.0\ \Omega is connected between the axle and the rim through sliding contacts (the resistances of the disc and the contacts are negligible). A light string wound on the axle, of radius r=0.10 mr=0.10\ \mathrm{m}, carries a mass m=0.50 kgm=0.50\ \mathrm{kg} that descends and finally reaches a constant speed. Take g=10 m s−2g=10\ \mathrm{m\,s^{-2}}. Find the final angular speed of the disc in rad s−1\mathrm{rad\,s^{-1}}.
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Answer: 8

When the disc turns at ω\omega, each radial element sees v=ωxv=\omega x, so the emf between axle and rim is ε=∫0aBωx dx=12Bωa2\varepsilon=\int_0^aB\omega x\,dx=\tfrac12B\omega a^2 and the current is i=ε/Ri=\varepsilon/R. The magnetic force on the radial current has torque τB=∫0aiBx dx=12iBa2=B2a4ω4R\tau_B=\int_0^aiBx\,dx=\tfrac12iBa^2=\dfrac{B^2a^4\omega}{4R}, opposing the rotation. At constant speed this balances the torque of the hanging mass, mgrmgr. So ω=4mgrRB2a4=4×0.5×10×0.1×14×0.0625=20.25=8 rad s−1\omega=\dfrac{4mgrR}{B^2a^4}=\dfrac{4\times0.5\times10\times0.1\times1}{4\times0.0625}=\dfrac{2}{0.25}=8\ \mathrm{rad\,s^{-1}}. As a check, i=12×2×8×0.25=2 Ai=\tfrac12\times2\times8\times0.25=2\ \mathrm{A} and i2R=4 W=mg (ωr)=5×0.8i^2R=4\ \mathrm{W}=mg\,(\omega r)=5\times0.8, so the heat generated equals the power of gravity.
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