Do non-inertial frames perceive a B field?

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SUMMARY

This discussion centers on the perception of magnetic fields (B fields) in non-inertial frames, specifically when an observer rotates on a turntable at the center of a charged ring. It concludes that while a rotating observer may perceive a B field due to their tangential velocity, the interpretation of electric and magnetic fields becomes complex in non-inertial frames. The electromagnetic tensor transforms as a tensor, allowing for the calculation of forces on test charges, but the distinction between electric and magnetic components is ambiguous. Ultimately, the discussion emphasizes that the concept of a "non-inertial frame" is misleading and should be approached through local observer congruences instead.

PREREQUISITES
  • Understanding of electromagnetic fields, specifically the relationship between electric (E) and magnetic (B) fields.
  • Familiarity with Lorentz transformations in the context of special relativity.
  • Knowledge of non-inertial reference frames and their implications in physics.
  • Basic comprehension of Minkowski coordinates and frame fields in general relativity.
NEXT STEPS
  • Study the implications of rotating reference frames in electromagnetism.
  • Learn about the electromagnetic tensor and its transformation properties.
  • Explore the concept of frame fields in general relativity and their applications.
  • Investigate the relationship between acceleration, rotation, and perceived forces in non-inertial frames.
USEFUL FOR

This discussion is beneficial for physicists, particularly those specializing in electromagnetism and relativity, as well as students seeking to deepen their understanding of non-inertial frames and their effects on electromagnetic perception.

cragar
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Lets say I am standing in the middle of a charged ring. And I am standing on a turn table.
Now I start to rotate in the center. From my point of view do I perceive a B field.
I mean I would have a velocity component.
 
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If you mean is there a B field in your reference frame then yes a compass would be messed up sitting in the center, but assuming that the radius of the ring is huge compared to you, you won't feel a magnetic force since your rotation doesn't really produce a velocity vector (again assuming you are vanishingly small compared to the ring radius).
 
To compute the B field would I just say that the ring is moving we an angular speed and do it that way.
 
Your point of view is non inertial. It is not even clear what is meant by "magnetic field" in non inertial frames.
 
so its not easy to calculate if we even can.
 
The EM tensor transforms as a tensor, so it is "relatively" easy to calculate the force on a test charge in your non-inertial frame. It is not clear how much of that force to attribute to electric field and how much to attribute to magnetic field because the electric and magnetic fields are components of the tensor in an inertial frame. In non-inertial frames interpreting certain components as this or that becomes suspect.
 
There is no such thing as a "noninertial frame". Because a "frame" covers the entire space, and noninertial coordinates must be treated locally. What a rotating observer sees is determined by a different Lorentz transformation at each point.

At the exact center of the ring, E = B = 0, and you can Lorentz transform it all you want, you still get zero.

At a distance r from the center there will be a net radial E field, and a rotating platform will have a tangential velocity v = ωr. An observer moving along with the platform at this point will see a B field, B = -v/c x E, pointing upward.
 
Bill_K said:
There is no such thing as a "noninertial frame".
That would be news to a very large number of peer reviewed authors.
 
So the B field would be B = -v/c x E, pointing upward. as Bill K said.
So If I had a charged sphere And I was driving around it in a circle I could just use this.
And this would give me the same B field as if the charged sphere was rotating.
 
  • #10
"There is no such thing as a noninertial frame."
That would be news to a very large number of peer reviewed authors.
I certainly wouldn't approve a paper that used the term. The word "frame" specifically applies to a set of Minkowski coordinates, and its inappropriate use leads to much of the confusion surrounding rotation and/or acceleration in relativity. The correct description is in terms of a timelike congruence of local observers, one through each point. They will necessarily have different velocities, and therefore do not form a single "frame of reference".
 
  • #11
Bill_K said:
The word "frame" specifically applies to a set of Minkowski coordinates
That is quite different from my understanding of the term. However, I must admit that my understanding comes from Wikipedia and PF:
http://en.wikipedia.org/wiki/Frame_fields_in_general_relativity
https://www.physicsforums.com/showthread.php?t=168631

According to my understanding the word "frame" refers specifically to a "frame field" which is a set of four orthonormal vectors at each point in the manifold. These vectors are not coordinates and integral curves of the timelike vectors may not be geodesics. When they are not then the frame is non-inertial.
 

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