Can Magnetic Forces Do Work on Charged Particles and Magnetic Dipoles?

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SUMMARY

The discussion centers on the work done by magnetic forces on charged particles and magnetic dipoles, particularly in the context of quantum mechanics and classical electromagnetism. It highlights that the Hamiltonian of a charged particle in a magnetic field includes a term for intrinsic magnetic moment, represented as -&vec;μ · &vec;B. Participants debate whether magnetic fields can perform work on particles, especially in scenarios like the Stern-Gerlach experiment, and whether energy conservation holds when magnetic dipoles interact. The conclusion drawn is that while classical electromagnetic principles may not apply, magnetic forces can indeed do work on magnetic dipoles.

PREREQUISITES
  • Understanding of the Dirac equation and its implications in quantum mechanics.
  • Familiarity with Hamiltonian mechanics and intrinsic magnetic moments.
  • Knowledge of the Stern-Gerlach experiment and its significance in quantum physics.
  • Concepts of energy conservation in both classical and quantum contexts.
NEXT STEPS
  • Explore the implications of the Dirac equation in nonrelativistic quantum mechanics.
  • Study the role of intrinsic magnetic moments in quantum systems.
  • Investigate the mechanics of the Stern-Gerlach experiment and its outcomes.
  • Research energy conservation principles in quantum mechanics versus classical physics.
USEFUL FOR

Physicists, quantum mechanics students, and researchers interested in the interactions of magnetic fields with charged particles and dipoles, as well as those exploring the nuances of energy conservation in quantum systems.

da_willem
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from the Dirac equation one can straightforwardly derive that in the nonrelativistic limit, the Hamiltonian of a charged particle in a magnetic field acquires a term

-\vec{\mu} \cdot \vec{B}

which shows the particle has an intrinsic magnetic moment (by analogy with the classical expression of the energy of a magnetic dipole in a magnetic field). Contrary to the classical case however, this moment is not sustained by a current (at least that is not the mainstream thought).

Now, looking at this classically the energy of an electron in a magnetic field causes a force if the field is inhomogeneous

\vec{F}=-\nabla(-\vec{\mu} \cdot \vec{B})=\nabla(\vec{\mu} \cdot \vec{B})

So the electron starts moving right? Now what force is responsible for this movement, who does the work?
 
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cesiumfrog said:
Does the magnetic field in the Stern-Gerlach experiment do work on an electron?

da_willem said:
I think a that here we should change our language and no longer speak of a force, as there is no such thing in quantum mechanics.

So you've changed your mind?

Regards force, I was content with the answer that we cannot expect results from classical EM to hold in the limit where classical EM fails.

Regards work, I presume it is energetically favourable (for whatever apparatus that provides the eternal magnetic field) if any stray dipoles are shifted aside, and the exact mechanism in that macroscopic apparatus (as per the previous thread) will turn out not to be directly magnetic.
 
So you think that in the process of moving the spin, the magnetic field decreases (field energy converted to kinetic energy) and that the source of the magnetic field is what's doing the work?

But then what if this magnetic field is also quantum mechanical in origin, like in the case of the hyperfine splitting. Here the (inhomogeneous) magnetic field of one spin interacts with the 'dipole moment' of another spin to form an interaction energy.

Suppose we can 'switch of' other interactions, I suppose these spins start moving. Where does this kinetic energy come from, as demanded by energy conservation? Classically the dipole moment can diminish, converting the kinetic energy of the charges generating the moment into translational motion. Qunatum mechaniclly however, the spins of a particle can't change, so where does this kinetic energy come from?

If the answer is, from the magnetic field energy, then isn't this exactly what can't happen classically: magnetic field energy > kinetic energy = magnetic work?!

Or does this (even classically) only hold for charges and the magnetic Lorentz force, and can one think of instances where classical magnetic moments start moving by converting magnetic field energy into kinetic energy?!
 
I think that from the perspective of whatever creates the external force, there is no difference between intrinsic magnetic dipole and a classical current loop. As such, in accelerating the dipole, the external apparatus should do work and (per the previous thread) this loss of energy may be attributed to something entirely other than the magnetic field itself.

But from the perspective of the elementary point particle, to the extent that we can speak about force and the like, work must be done by the magnetic field because there are apparently no other internal components through which to attribute the increase in energy. Anyway, that's my take on it.
 
cesiumfrog said:
I think that from the perspective of whatever creates the external force, there is no difference between intrinsic magnetic dipole and a classical current loop. As such, in accelerating the dipole, the external apparatus should do work and (per the previous thread) this loss of energy may be attributed to something entirely other than the magnetic field itself.

But I'm not talking about any external force, just two spins in a vacuum. I didn't do the classical calculation, so I'm not sure if they even start to move due to the inhomogeneous fields they posses, but if they do, where does the energy come from?!
 
da_willem said:
just two spins in a vacuum. [..] if they do [start moving], where does the energy come from?!

This is hand-wavy, but.. If the two magnetic fields add linearly, and the energy of the field is proportional to the square, would that suffice?
 
So, I guess my point is, magnetic forces can do work, maybe not on charged particles by the magnetic part of the Lorentz force, but on magnetic dipoles they can!
 

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