EM Faraday tensor transformation for conductor carrying current

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Discussion Overview

The discussion revolves around the transformation of the electromagnetic Faraday tensor in relation to a conductor carrying current, particularly focusing on the differences in electric and magnetic fields observed in different inertial reference frames. Participants explore the implications of Lorentz transformations on charge distribution and field perception in these frames.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants note that in the Lab frame, there is only a magnetic field around the wire due to the current, while in the frame where electrons are at rest, an electric field arises due to Lorentz contraction affecting charge balance.
  • Others argue that different frames will not agree on the net charge of the wire, as the perception of charge flow and distribution changes with the observer's frame of reference.
  • A participant questions whether a deficiency of electrons at one end and an excess at the other is necessary to initiate current flow in the wire.
  • Another participant describes how, in a frame where positive charges are at rest, the negative charge density decreases due to lack of contraction, while the positive charge density increases, leading to a charged wire in that frame.
  • Some participants discuss the notion that the charge of the wire can be chosen arbitrarily in any frame, suggesting that the assumption of a neutral wire in the Lab frame accounts for the effects of moving charges.
  • There is a suggestion that relativity connects the observations of different observers regarding the same physical situation, but does not dictate how the fields are established.

Areas of Agreement / Disagreement

Participants express differing views on the nature of charge distribution in various frames, with no consensus reached on the implications of these transformations for the understanding of electric and magnetic fields in conductors.

Contextual Notes

Participants highlight that the discussion involves assumptions about charge distribution, the nature of current flow, and the establishment of electromagnetic fields, which remain unresolved and contingent on the chosen frame of reference.

cianfa72
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TL;DR
Analysis of EM Faraday tensor transformation in the context of conductor carrying current.
Hi, starting from a recent thread, I'd like to discuss a point related to the Lorentz transformation of EM Faraday tensor field between inertial reference frame.

As explained in this video at minute 11:20, in the Lab inertial frame there is only a magnetic field B in the region surrounding the wire due to the current of electrons flowing inside the wire. There is not electric field since, inside each volume/section in the wire, the net charge is zero.

The video explains that instead, in the inertial frame where the electrons are at rest, on a external positive charge (ione proton) at rest in such frame actually acts a Lorentz force due to an Electric field E. This because the Lorentz contraction charges inside the wire are not longer balanced.

My doubt is whether there is or not a symmetry in the analysis done in the two frames.

Namely if in the Lab frame there is a balance of electrons and positive metal ions inside the wire, why it is not longer the case in the other frame where electrons are at rest and positive ions move in the opposite direction with the same speed ?
 
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If there's only a single long straight wire then there must be a pool of charge at each end and if one frame says charge started flowing from both ends simultaneously then another frame won't agree. So they won't agree about the net charge on the wire.

If you have a circuit with a battery then you can't have a single straight wire, you must have a loop. If you have an excess of charge on one side of the loop you'll have a deficit on the other. Again, the difference between frames will be traceable to different ideas about necessary electron density and velocity to keep supplying electrons to the other side of the loop.
 
Ibix said:
If there's only a single long straight wire then there must be a pool of charge at each end and if one frame says charge started flowing from both ends simultaneously then another frame won't agree. So they won't agree about the net charge on the wire.
Sorry, do you mean that a deficiency of electrons at a side and an excess of them at the other side are actually required to start a current inside the wire ?
 
cianfa72 said:
Sorry, do you mean that a deficiency of electrons at a side and an excess of them at the other side are actually required to start a current inside the wire ?
If the current is flowing only in one direction then there has to be a source of electrons at one end.
 
For the infinite wire consider two frames. The first is at rest wrt the positive charges with the negative ones drifting slowly to the right. In this frame there is only a magnetic field and the wire is neutral. Now boost along the wire at the drift rate putting the negative charges at rest. The negative charge per unit length in this second frame will decrease because it’s no longer contracted while the positive charge density will increase because it’s now contracted in this new frame. This results in the wire being charged in the second frame.

So, the real question is, why is the wire neutral in the first frame?
 
Paul Colby said:
So, the real question is, why is the wire neutral in the first frame?
Exactly, but sorry I don't know why....
 
well the charge of the wire in the first (or any) frame is a choice. One is permitted to charge the wire or not. People who came up with this problem chose neutral wires in the rest frame.
 
Paul Colby said:
well the charge of the wire in the first (or any) frame is a choice. One is permitted to charge the wire or not. People who came up with this problem chose neutral wires in the rest frame.
Ah ok, so in a sense choosing zero for the net charge of the wire in Lab frame, already takes in account the contraction of electrons moving with drift velocity.
 
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Ibix said:
If the current is flowing only in one direction then there has to be a source of electrons at one end.
Ok, so in this case your point is that two different inertial frames won't agree on when electrons on both wire's end sides simultaneously start to move. Hence at any point in time (w.r.t. a given frame respectively) the net charge in the wire won't be the same.

Therefore if the net charge is assumed to be zero in the Lab frame, then it will not be the case in the frame in which moving electrons are at rest.
 
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  • #10
cianfa72 said:
Ok, so in this case your point is that two different inertial frames won't agree on when electrons on both wire's end sides simultaneously start to move. Hence at any point in time (w.r.t. a given frame respectively) the net charge in the wire won't be the same.
So, relativity only connects what two observers will see of the same physical situation. The situation here are the fields about the wire. I've assumed these fields are static (not time dependent) in either frame. There is no "start moving" unless one is discussing how these fields are established in the first place. Relativity doesn't dictate how these fields are established. The potential of the wire in the lab frame relative to infinity may be chosen at will. Each different potential yields a different radial electric field in the Lab.
 

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