Length contraction in a current carrying wire?

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Discussion Overview

The discussion revolves around the concept of length contraction in a current-carrying wire and its implications for the wire's electrical neutrality from different reference frames. Participants explore the relationship between charge density, electric fields, and relativistic effects, questioning how these factors interact in both stationary and moving frames.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that a current-carrying wire is electrically neutral in its rest frame, while others question how this neutrality can be maintained when considering length contraction of electrons versus stationary positive charges.
  • One participant expresses confusion about the implications of length contraction, suggesting that it should lead to a net electric field due to differing contractions of electrons and protons.
  • Another participant emphasizes that the neutrality of the wire is an experimental fact and should be treated as a boundary condition in the problem, rather than something derived from first principles.
  • Some participants discuss the mathematical derivations related to the forces acting on charges in the wire, questioning the assumptions made in equating electric and magnetic forces in certain contexts.
  • There are mentions of the role of non-simultaneity versus Lorentz contraction in explaining the behavior of charges in a moving frame.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of length contraction for the neutrality of a current-carrying wire. Multiple competing views remain regarding how charge densities and electric fields are perceived in different reference frames.

Contextual Notes

Some participants highlight limitations in understanding the relationship between charge density and relativistic effects, noting that the discussion involves assumptions about the behavior of charges under different conditions. The complexity of the mathematical relationships involved is acknowledged but not resolved.

  • #61
Which is roughly the same answer I’ve given in post #44 .

So what’s the difference between us? I want to know why the –ve charge density doesn’t increase in a non moving lab frame, not even for the most massive currents. You are apparently happy to accept the facts and to get on with life. (perhaps not a bad idea).
 
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  • #62
I still don't understand your confusion on this point. Again, there is no lattice for the electrons so they are free to take any spacing that satisfies the laws and the boundary conditions.

You seem to understand that everything in the lab frame follows Maxwell's equations, and you seem to understand that when you Lorentz transform into the "drift" frame you get correct results in that frame also. Do you possibly think that Maxwell's equations should be violated in the lab frame for large currents?

I don't think it is a matter of me being happy to accept the facts. The facts are empirical data and there is never any question of accepting them or not; you must accept them or you are not doing science. In my mind the point is that the theories fit the facts and that is what makes me happy to accept the theories and get on with life.
 
  • #63
DaleSpam said:
there is no lattice for the electrons so they are free to take any spacing that satisfies the laws and the boundary conditions.

You seem to understand that everything in the lab frame follows Maxwell's equations, and you seem to understand that when you Lorentz transform into the "drift" frame you get correct results in that frame also.
That almost sounds that you could go along with the statement that in a drift frame conduction electrons are spread out.
 
  • #64
Certainly. The distance between conduction electrons in the drift frame is larger than the distance between electrons in the lab frame. In fact, the distance between electrons in the drift frame is larger than the distance between electrons in any other frame since the proper distance is always greater than or equal to the coordinate distance.
 
  • #65
Just some thoughts.

In their rest frame the conduction electrons must all move apart a little and therefore end up forming a longer length than the lattice. In the lab frame this expansion is not observed but it must be there in the drift frame to start with. These electrons see the lattice contracted but they still feel a force somehow which moves them apart. How do the electrons know how far to move? What force drives them apart?
 
  • #66
Per Oni said:
How do the electrons know how far to move? What force drives them apart?
The EM-field (Maxwell's equations, especially Gauss' law). Just like in the lab frame.
 
Last edited:

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