Discussion Session for PHY2049 Physics with Calculus 2 - Electromagnetism Spring 2012 Week # 8 Problem 3 The figure shows a wood cylinder of mass m = 0.25 kgs and length L = 0.1 m, with N = 10 turns of wire wrapped around it longitudinally, so that the plane of the wire coil contains the long central axis of the cylinder. The cylinder is released on a plane inclined at an angle θ to the horizontal, with the plane of the coil parallel to the incline plane. If there is a vertical uniform magnetic field of magnitude 0.5 T, what is the least current i through the coil that keeps the cylinder from rolling down the plane? Solution The first thing we need to remember comes from physics I: the problem demands translational and rotational equilibrium. The former implies that the net force on the cylinder should be equal to zero while the latter means that the net torque is equal to zero as well. Using the first equation should give us the limiting value the current must have so that the cylinder remains still. Let fs be the force of static friction acting on the contact point between the cylinder and the inclined plane. This is one the forces that makes it rotate. The other one is the force produced by the electric current interacting with the external magnetic field. The net force is: mg sin θ − fs = ma (1) The question is now, how do we relate this to the electric current? We see that the only unknown variable here is fs , therefore the current must be implicit in the variable fs . We now move to rotational equilibrium which is ~τnet = 0 where ~τnet is the 1 net torque acting on the cylinder. There are two sources of torque acting in opposite directions of rotation: the force of friction tries to make the cylinder to roll down while the currrent creates a torque that tries to make it go uphill. This in other words means that the torque due to these forces are opposite in sign. We can write this as τnet = τf riction − τcurrent (2) On one hand we know that τf riction = fs r where r is the radius of the cylinder (notice that this was not given in the problem, so it better cancels out in the end). On the other hand, you learned this week that the torque produces by a loop of current is ~ ~τcurrent = µ ~ ×B ~ is the external magnetic field and µ where B ~ is the magnetic moment defined as |~ µ| = iAN where i, A and N are the current, the area, and the number of turns of the loop respectively. The direcction of this µ ~ vector is the direction perpendicular to the plane of the loop. Since the direction of the external magnetic field is fixed and pointing up, we have ~ = µB sin θ = iA B sin θ N = i 2rL B sin θN τcurrent = |~ µ × B| where we used the fact that the area A of the loop of current is A = 2rL because the loop is a rectangle of sides L and 2r. We have also used the ~ is fact that the angle θ that is necessary to compute the cross product µ ~ ×B precisely the same angle θ that the inclined plane does with the horizontal. Putting this into (2) we have f r =i 2rL B sin θN f =i 2L B sin θN (3) where we notice the r canceled out as expected. Since we want the net force being equal to zero, i.e. the acceleration a must be zero, from (1) we have: f = mg sin θ. Plugging this into (3) we obtain i= mg 0.25 × 9.8 = = 2.45 A 2N LB 2 × 10 × 0.1 × 0.5 2 (4)