A moving magnet in a linear electric field

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SUMMARY

The discussion centers on the effects of a moving magnet in an electric field, contrasting it with the established behavior of charged masses in magnetic fields. It highlights the lack of experimental exploration in this area, suggesting that a groundbreaking experiment could be conducted, akin to those of 19th-century physicists. The conversation references the Heaviside equations and the complexities surrounding magnetic charge and electric dipole moments, indicating that existing literature presents conflicting interpretations. The conclusion emphasizes the need for further investigation into the behavior of permanent magnets in various inertial frames.

PREREQUISITES
  • Understanding of electromagnetic theory, particularly the Lorentz force law.
  • Familiarity with the Heaviside equations and their implications in electromagnetism.
  • Knowledge of Minkowski tensors and their role in relativistic electrodynamics.
  • Basic principles of electric dipole moments and magnetic polarization.
NEXT STEPS
  • Conduct experiments involving the motion of a bar magnet between large capacitor plates.
  • Research the implications of the Heaviside equations on magnetic charge and force.
  • Explore the relationship between electric dipole moments and moving permanent magnets.
  • Study the role of Minkowski tensors in the context of electromagnetic fields and polarization.
USEFUL FOR

Physicists, electrical engineers, and researchers interested in advanced electromagnetism and the experimental exploration of magnetic and electric interactions.

GregM
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If a electrically charged mass travels thru a magnetic(m) field, it will accelerate at right angles to its velocity and the m-field. Under some conditions like this the charged mass will travel in a circular loop due to this magnetic force acceleration. This info is all over the internet. e.g.
https://courses.lumenlearning.com/b...on-of-a-charged-particle-in-a-magnetic-field/

What about a moving magnet in an electric field? A similar effect? Seems not a word has ever been written about it. Google returns nothing. Perhaps no-one has ever thought to do this experiment. Potential for a ground breaking 19th century style experiment here. Which one of us will be the neo Faraday? I wonder what the Heaviside equations predict.
 
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problem with the heaviside equations is they associate electric charge with mass, but not magnetic charge. Its harder to see how magnetic mass experiences force.
 
can't they just report the results of dropping a bar magnet between 2 large long capacitor plates? Debate about interpretation of the results should come later.
 
https://link.springer.com/article/10.1140/epjp/i2014-14215-y
https://iopscience.iop.org/article/10.1088/0143-0807/32/4/003/meta
https://iopscience.iop.org/article/10.1088/0143-0807/33/1/L02
https://iopscience.iop.org/article/10.1088/0143-0807/33/1/L03/meta

Those papers contradict each other because they're all wrong. A magnetic would require an inhomogeneous magnetic field to feel a force. There are some papers claiming that a moving magnet acquires an electric dipole moment, but they are also wrong.
 
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But the latter is correct. If you have a permanent magnet and view it from an inertial frame, where it's moving there's also an elecctric dipole moment. It's because the electric and magnetic polarizations of a medium are components of an antisymmetric 2nd-rank Minkowski tensor in a similar way as the electric and the magnetic field are components of such an antisymmetric tensor. The only difference is that due to the historical misconception of magnetization there's a sign change. So you have
$$F^{0j}=-F^{j0}=-E^j, \quad F^{jk}=-\epsilon^{jkl} B^l$$
and
$$P^{0j}=-P^{j0}=p^j, \quad P^{jk}=+\epsilon^{jkl} m^l,$$
where ##\vec{E}## are the electric, ##\vec{B}## the magnetic field components and ##\vec{p}## the electric and ##\vec{m}## the magnetic polarization of the matter.

Thus an uncharged permanent magnet which has only a magnetization in its rest frame has both an electric polarization and a magnetization in any other inertial frame.
 
"the electric and magnetic polarizations of a medium are components of an antisymmetric 2nd-rank Minkowski tensor"
There's no proof of that for a permanent magnet.
 
That's standard relativistic electrodynamics.
 
I didn't realize that was the proof.
 

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