Week #8 Problems
Solution. The component of the velocity of the bar that is perpendicular to the magnetic field is vcos θ, so the induced emf is E = BLvcos θ This produces a current in the wire I = E /R = (BLvcos θ)/R into the page. Because the current is perpendicular to the magnetic field, the force on the wire from the magnetic field will be horizontal as shown, with magnitude FB = ILB = (B2L2vcos θ)/R For the wire to slide down at a steady speed, the net force must be zero. If we consider the components along the rail, we have FBcos θ - mgsin θ = 0, or [(B2L2vcos θ)/R]cos θ = B2Lvcos2 θ)/R = mgsin θ (0.55 T)2(0.30 m)2v(cos2 5°)/(0.60 Ω) = 0.040 kg)(9.8 m/s2)sin5°, which gives v = 0.76 m/s. |
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