Do non-inertial frames perceive a B field?

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Discussion Overview

The discussion revolves around the perception of a magnetic field (B field) from a non-inertial reference frame, specifically in the context of a charged ring and an observer rotating at its center. Participants explore the implications of non-inertial frames on electromagnetic fields, the calculation of these fields, and the definitions of reference frames in physics.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions whether a rotating observer in the center of a charged ring perceives a B field, suggesting that they would have a velocity component.
  • Another participant asserts that while a compass would be affected, the observer would not feel a magnetic force due to their rotation, assuming they are small compared to the ring radius.
  • A participant proposes calculating the B field by considering the ring's angular speed.
  • Concerns are raised about the clarity of defining a "magnetic field" in non-inertial frames, with one participant stating that it complicates calculations.
  • Discussion includes the transformation properties of the electromagnetic tensor and the difficulty in attributing forces to electric or magnetic fields in non-inertial frames.
  • One participant argues against the existence of a "non-inertial frame," stating that such frames must be treated locally and that the behavior of rotating observers is determined by different Lorentz transformations at each point.
  • Another participant agrees with the assertion that at the center of the ring, both electric and magnetic fields are zero, while noting that at a distance from the center, there would be a net electric field and a perceived B field due to tangential velocity.
  • One participant reiterates the formula for the B field as derived from the electric field, suggesting it could be applied to a charged sphere being circled.
  • Disagreement arises regarding the definition of "frame," with some participants emphasizing the need for precise terminology in the context of relativity and others referencing different understandings from literature.

Areas of Agreement / Disagreement

Participants express multiple competing views on the existence and definition of non-inertial frames, the interpretation of electromagnetic fields in such frames, and the appropriate terminology to use. The discussion remains unresolved with no consensus reached.

Contextual Notes

Participants highlight limitations in defining magnetic fields in non-inertial frames and the challenges of applying Lorentz transformations. There are also references to differing interpretations of what constitutes a "frame" in the context of relativity.

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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