A long solenoid of radius carries a current that is being changed so that its uniform…

PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Electric current and circuits · Electromagnetic induction and alternating-current circuits

Electricity, Magnetism and Electromagnetism, Ch Faraday's law, motional emf and Lenz's law

Problem

A long solenoid of radius R=3.0 cmR = 3.0\ \mathrm{cm} carries a current that is being changed so that its uniform interior field, directed along the axis, grows at the steady rate dB/dt=0.80 T s−1dB/dt = 0.80\ \mathrm{T\,s^{-1}}. The field outside the solenoid is negligible. Look along the axis so that B\mathbf{B} points out of the page. A circular ring of wire of radius 6.0 cm6.0\ \mathrm{cm}, coaxial with the solenoid and in a plane perpendicular to the axis, is made of two resistors joined at diametrically opposite points PP (at the top of the view) and QQ (at the bottom): a 220 Ω220\ \Omega resistor forms the right-hand half of the ring and a 680 Ω680\ \Omega resistor the left-hand half. The connecting wire has negligible resistance. ((a)) Explain why the current that appears in this stationary ring cannot be driven by a magnetic force on its carriers, and, using a circular path coaxial with the solenoid together with the symmetry of the arrangement, derive the magnitude of the induced electric field at a radius s<Rs < R. Evaluate it at the solenoid's surface, s=Rs = R. ((b)) Find the emf round the ring, and the current in it, stating its sense in the view described. ((c)) Two ideal voltmeters (drawing no current) are each connected to PP and QQ with the ++ lead on PP. The leads of the first run close alongside the right-hand (220 Ω220\ \Omega) half of the ring, those of the second close alongside the left-hand (680 Ω680\ \Omega) half, so that in each case the loop formed by meter, leads and that half of the ring encloses negligible flux from the solenoid. Give the signed reading VP−VQV_P - V_Q of each meter, show that the two readings differ by the emf, and say what this proves about the induced field.

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