Originally Posted by eJavier
All I'm saying is this: the force on a magnetc dipole is derived from the Loretz force law, which means that the magnetic force does not work.
|
All I'm saying is that's just wrong. If you have say a uniform field

and a magnet with dipole moment

, you have to do work to pull it out of alignment with B. The
torque to do this is

.
There is a
potential energy U:

.
Rotating the dipole out of alignment increases the potential energy. Let it go and it will rotate on its own as the potential energy decreases and the rotational
kinetic energy increases. This is known as doing work. The magnetic field is doing work on the dipole, just as gravity does work on a mass that is falling. These formulas are directly from Jackson. Lorentz force is not relevant here. You are mis-applying something else, namely that a magnetic field does no work on a charged particle.
The point I'm trying to make is that Lorentz force law implies no work done by the magnetic force. Reading your posts I get the impression that you're saying that it's only valid for electric charges (ie. Lorentz force law), so I would like you to show me a formula for a force between an electric field and something other than an electric current.
|
Did you mean magnetic field?
Anyway, the force law between two magnetic poles p_1 and p_2 in free space is this
in the direction of the vector r from p_1 to p_2. This can be described as p_2 in the magnetic field
of p_1. Equally well, describe it by a potential

.
So you complain that monopoles don't exist. Fine. They only come in pairs. The potential from an isolated dipole is found be adding the two together:

,
where

is the separation of the two opposite poles

, and

is the angle it makes with the observation point. We call

the dipole moment m. So

.
This is the same as the formula given by Jackson.
If you have a cylindrical permanent magnet, with magnetization

, then it acts to a very good approximation as if it has magnetic monopoles on its North surface with a charge density

, with a surface charge density of exactly opposite sign at the South pole (this is directly from Jackson...). Get two such magnets together and they attract or repel eachother with forces given by applying the formula for F that I gave above to these surfaces and integrating. These forces have potentials and everything, just as in gravity and electrostatics.
Here's a quote from my first post "Hold two magnets apart; now they have potential energy. Let them go; now the field does work on the magnets and the result is that they accelerate towards one another." Sheesh. I'm repeating myself...