Highschool student trying to write a lab report. Why does eddy current braking seem to decrease exponentially with magnet distance?
I've been doing a small experiment with eddy current braking and I'm confused about the theory.
The setup is pretty simple: an aluminum disk is spun using a rotary motion sensor, and I hold a stationary rectangular neodymium magnet above the disk. The only thing I change is the vertical distance between the bottom of the magnet and the top of the disk (2 cm to 4 cm). I then measure the angular deceleration over the same angular velocity interval each time (20–25 rad/s).
The average decelerations I got were roughly:
- 2.0 cm → 20.24 rad/s^(2)
- 2.5 cm → 12.63 rad/s^(2)
- 3.0 cm → 5.99 rad/s^(2)
- 3.5 cm → 3.09 rad/s^(2)
- 4.0 cm → 1.92 rad/s^(2)
The weird thing is that an exponential trendline fits almost perfectly (R^(2) ≈ 0.99).
I understand the basic mechanism:
- changing flux induces eddy currents,
- the eddy currents create a magnetic field opposing the change,
- the interaction with the permanent magnet creates the braking torque.
I've also seen derivations that the braking force is proportional to vB^(2), so the magnetic field is clearly the important quantity.
What I don't understand is where an exponential dependence on separation would come from physically.
Most explanations I find assume the magnet behaves like a dipole and use something like B**∝**1/r^(3), but my magnet is a rectangular neodymium magnet and the distances are only 2–4 cm from the disk, so I'm not sure that approximation is even valid.
Is there a better expression for the magnetic field of a permanent magnet in this regime? Or is it more likely that the exponential fit is just approximating the actual field over a small range of distances?
I'm mainly looking for the physics behind it rather than curve-fitting advice. If anyone knows a derivation or a good reference on eddy-current brakes with permanent magnets, I'd really appreciate it.