Feynman: Relativity of Magnetic and Electric Fields

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Discussion Overview

The discussion revolves around the relativity of magnetic and electric fields as presented by Feynman, focusing on the implications of charge density transformations in different reference frames. Participants explore the concepts of charge density, drift velocity, and the relativity of simultaneity, while considering various illustrative scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants express confusion over the notation used by Feynman, particularly the re-use of ##\rho_\omicron##, suggesting it leads to misunderstandings about charge densities.
  • There is a discussion on the average "drift" velocity of electrons and how it relates to charge density in different frames.
  • Participants note that the conduction electron density is lower in the frame moving with the electrons compared to the rest frame of the wire, while the positive charge density increases in the electron rest frame.
  • Some participants propose that the proportion of electrons to protons changes when measured in different reference frames, questioning whether this is influenced by the relativity of simultaneity.
  • A hypothetical scenario involving a negatively charged moving train in a positively charged tunnel is discussed to illustrate these concepts, with participants analyzing the implications of Lorentz contraction from different frames of reference.
  • Some participants agree that the proposed scenario is a good informal summary of Feynman's treatment of the topic.
  • Additional resources are shared, including links to alternative treatments of the topic and classic presentations for undergraduates.

Areas of Agreement / Disagreement

Participants generally agree on the confusion surrounding the notation and the implications of charge density transformations, but there is no consensus on the correctness of the proposed scenarios or the interpretations of simultaneity. Multiple competing views remain regarding the implications of these concepts.

Contextual Notes

Participants acknowledge the complexity of the topic, including the dependence on different reference frames and the potential for misunderstanding due to notation. The discussion reflects ongoing exploration rather than settled conclusions.

Hetware
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The diagrams aren't coming through on my system, but the text is readable:

http://books.google.com/books?id=hlRhwGK40fgC&pg=SA13-PA6&lpg=SA13-PA6&#v=onepage&q&f=false

First off, I'm pretty sure he re-uses ##\rho_\omicron## to mean different things at different points in the discussion. That was very confusing to me. It gives the impression that ##\rho_\omicron=\rho_+=\rho^{'}_{-}## which is incorrect.

I do understand that the velocity of attributed to the electrons is an average "drift" velocity.

I believe I finally figured this out. To an extent. Eq. 13.24 and eq 13.26 tell us that the conduction electron density is lower in the frame moving along with the electrons than it is in the rest frame of the wire. At the same time the positive charge density at rest relative to the wire becomes greater when transformed to the electron rest frame.

That means the proportion of electrons to protons in the wire is different when measured in relatively moving reference frames. Does this depend on the relativity of simultaneity?

Could this be demonstrated by placing a uniformly negatively charge moving train in a uniformly positively charged tunnel and adjusting the relative charge so that the electric field at rest with respect to the tunnel vanishes.

Assume at a given instant the entire train is just inside the tunnel as viewed from the tunnel rest frame. So the train appears Lorentz contracted. Now if we run along with the train, the tunnel will appear Lorentz contracted, and there will never be a time in the train's inertial frame when the entire train is in the tunnel. The event of the front for the train reaching the end of the tunnel will precede the event of the end of the train passing the beginning of the tunnel.

In the tunnel rest frame both events occur at the same time.

I recall reading something that discouraged that line of reasoning, but I don't see how it's wrong.
 
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Hetware said:
The diagrams aren't coming through on my system, but the text is readable:

http://books.google.com/books?id=hlRhwGK40fgC&pg=SA13-PA6&lpg=SA13-PA6&#v=onepage&q&f=false

First off, I'm pretty sure he re-uses ##\rho_\omicron## to mean different things at different points in the discussion. That was very confusing to me. It gives the impression that ##\rho_\omicron=\rho_+=\rho^{'}_{-}## which is incorrect.

I'm pretty sure that \rho_\omicron is the charge density in the rest frame of the charges. The only confusion here is that this will be a different frame for the electrons than the protons, because they have different rest frames.

I do understand that the velocity of attributed to the electrons is an average "drift" velocity.

I believe I finally figured this out. To an extent. Eq. 13.24 and eq 13.26 tell us that the conduction electron density is lower in the frame moving along with the electrons than it is in the rest frame of the wire. At the same time the positive charge density at rest relative to the wire becomes greater when transformed to the electron rest frame.

That means the proportion of electrons to protons in the wire is different when measured in relatively moving reference frames. Does this depend on the relativity of simultaneity?

Yes, indeed it does.

Could this be demonstrated by placing a uniformly negatively charge moving train in a uniformly positively charged tunnel and adjusting the relative charge so that the electric field at rest with respect to the tunnel vanishes.

That's a good informal summary of what Feynman just did, don't you think?

Assume at a given instant the entire train is just inside the tunnel as viewed from the tunnel rest frame. So the train appears Lorentz contracted. Now if we run along with the train, the tunnel will appear Lorentz contracted, and there will never be a time in the train's inertial frame when the entire train is in the tunnel. The event of the front for the train reaching the end of the tunnel will precede the event of the end of the train passing the beginning of the tunnel.

In the tunnel rest frame both events occur at the same time.

I recall reading something that discouraged that line of reasoning, but I don't see how it's wrong.

Offhand, I don't see anything wrong with it either.
 
Here is a more lowbrow treatment of the same topic: http://www.lightandmatter.com/html_books/0sn/ch11/ch11.html

The classic presentation of these ideas for undergraduates is in Purcell, Electricity and Magnetism.

It can also be done by boosting a loop rather than a straight wire: https://www.physicsforums.com/showthread.php?t=631446
 
Last edited by a moderator:
bcrowell said:
Here is a more lowbrow treatment of the same topic: http://www.lightandmatter.com/html_books/0sn/ch11/ch11.html

The classic presentation of these ideas for undergraduates is in Purcell, Electricity and Magnetism.

It can also be done by boosting a loop rather than a straight wire: https://www.physicsforums.com/showthread.php?t=631446

Bookmarked.
 
Last edited by a moderator:

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