1. Physics 2102 Lecture 14 Ch28: Magnetic Forces on Current Wires Physics 2102 Jonathan Dowling Star Quake on a Magnetar! “I’ll be back…. Aurora Borealis

2. Crossed Fields E vs. B F E =qE B E y q F B =vqBF E v L F E =ma => y=qEL 2 /(2mv 2 ) F B =F E => y=0 => v=E/B

3. Magnetic force on a wire. L Note: If wire is not straight, compute force on differential elements and integrate:

4. Example By symmetry, F 2 will only have a vertical component, Notice that the force is the same as that for a straight wire, LLRR and this would be true no matter what the shape of the central segment!. Wire with current i. Magnetic field out of page. What is net force on wire?

5. Example 4: The Rail Gun Conducting projectile of length 2cm, mass 10g carries constant current 100A between two rails. Magnetic field B = 100T points outward. Assuming the projectile starts from rest at t = 0, what is its speed after a time t = 1s? B I L Force on projectile: F= ILB (from F = iL x B) Acceleration: a = iLB/m (from F = ma) v(t) = iLBt/m (from v = v 0 + at) = (100A)(0.02m)(100T)(1s)/(0.01kg) = 2000m/s = 4,473mph = MACH 8! projectile rails

6. Torque on a Current Loop: Principle behind electric motors. Net force on current loop = 0 For a coil with N turns,  = N I A B sin , where A is the area of coil Rectangular coil: A=ab, current = i But: Net torque is NOT zero!

7. Magnetic Dipole Moment N = number of turns in coil A=area of coil. We just showed:  = NiABsin  Right hand rule: curl fingers in direction of current; thumb points along  Define: magnetic dipole moment  As in the case of electric dipoles, magnetic dipoles tend to align with the magnetic field.

8. Electric vs. Magnetic Dipoles -Q  QE +Q p=Qa