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Today’s agenda: Review and some interesting consequences of F=qvxB.

Today’s agenda: Review and some interesting consequences of F=qvxB. You must understand the similarities and differences between electric forces and magnetic forces on charged particles. Magnetic forces on currents and current-carrying wires.

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Today’s agenda: Review and some interesting consequences of F=qvxB.

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  1. Today’s agenda: Review and some interesting consequences of F=qvxB. You must understand the similarities and differences between electric forces and magnetic forces on charged particles. Magnetic forces on currents and current-carrying wires. You must be able to calculate the magnetic force on currents. Magnetic forces and torques on current loops. You must be able to calculate the torque and magnetic moment for a current-carrying wire in a uniform magnetic field. Applications: galvanometers, electric motors, rail guns. You must be able to use your understanding of magnetic forces and magnetic fields to describe how electromagnetic devices operate.

  2. Magnetic Forces and Torques on Current Loops We showed (not in general, but illustrated the technique) that the net force on a current loop in a uniform magnetic field is zero. No net force means no motion. No net force means no motion NOT. Example: a rectangular current loop of area A is placed in a uniform magnetic field. Calculate the torque on the loop. Let the loop carry a counterclockwise current I and have length L and width W. I L B The drawing is not meant to imply that the top and bottom parts are outside the magnetic field region. W

  3. There is no force on the “horizontal” segments because the current and magnetic field are in the “same” direction. There is no force on the “horizontal” segments because the current and magnetic field are in the “same” direction. Homework hint (know why). FL FR   L B I The vertical segment on the left “feels” a force “out of the page.” W The vertical segment on the right “feels” a force “into the page.” The two forces have the same magnitude: FL = FR = ILB. Because FL and FR are in opposite directions, there is no net force on the current loop, but there is a net torque. Let’s look “down” along the “green axis” I just drew.

  4. Top view of current loop, looking “down,” at the instant the plane of the loop is parallel to the magnetic field. FR B   IR IL In general, torque is FL area of loop = WL

  5. FR When the magnetic field is not parallel to the plane of the loop…  IR B    IL A FL Define A to be a vector whose magnitude is the area of the loop and whose direction is given by the right hand rule (cross A into B to get ). Then

  6. IA is defined to be the magnetic moment of the current loop. Magnetic Moment of a Current Loop FR  IR Alternative way to get direction of A: curl your fingers (right hand) around the loop in the direction of the current; thumb points in direction of A. B    IL A FL Homework Hint Your starting equation sheet has:

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