Is the Theory of Magnetism and Relativity Flawed?

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Discussion Overview

The discussion revolves around the relationship between magnetism and relativity, specifically examining the forces acting on charged particles in different frames of reference. Participants explore the implications of length contraction on the behavior of current-carrying wires and the resulting electric and magnetic fields, questioning established derivations and interpretations.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Exploratory

Main Points Raised

  • Some participants reference a derivation suggesting that the force on a negatively charged particle from a neutral current-carrying wire can be viewed as purely magnetostatic in one frame and purely electrostatic in another due to length contraction.
  • One participant expresses confusion about extending this idea to two current-carrying wires, noting that both should have positive charge and thus repel, contrary to expectations of attraction.
  • Another participant argues that the invariance of the electromagnetic field (E2 - B2) means that one cannot have purely electric or magnetic fields in different frames.
  • Some participants discuss the role of magnetic fields and their directions in determining forces on charged particles, referencing the Lorentz force equation.
  • A participant suggests that if both wires have positive charge, they should repel, but the attractive magnetic force could dominate, leading to an overall attractive interaction.
  • One participant challenges the validity of Feynman's derivation, claiming that it overlooks certain aspects of the electrostatic case, particularly the behavior of protons in different frames.
  • There is a discussion about whether both wires are length contracted or if only the electrons are moving, leading to differing interpretations of charge distribution.

Areas of Agreement / Disagreement

Participants express differing views on the validity of established theories and derivations, particularly regarding the interaction of electric and magnetic forces in relativistic contexts. There is no consensus on the correctness of the interpretations or the implications of the derivations discussed.

Contextual Notes

Some participants highlight limitations in the derivations referenced, including assumptions about charge distributions and the treatment of moving versus stationary charges. The discussion reflects ongoing uncertainties in the application of relativity to electromagnetic theory.

nassboy
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I've seen in feynman and on the internet a derivation that the force on a negatively charged particle from neutral current carrying wire can be shown to be purely magnetostatic in one frame of reference and purely electrostatic in the other frame of reference using the length contraction. The contracted wire has a net positive charge, and therefore attracts the negatively charged particle.

I've tried to extend this idea to two current carrying wires(the direction of the current the same in both wires)...but it seems that they both would have positive charge and repel when they should attract.

What am I doing wrong?
 
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nassboy said:
I've seen in feynman and on the internet a derivation that the force on a negatively charged particle from neutral current carrying wire can be shown to be purely magnetostatic in one frame of reference and purely electrostatic in the other frame of reference using the length contraction.

Hi nassboy! :smile:

That doesn't look right …

E2 - B2 is invariant (independent of the frame of reference), so you can't have the same field with just E or just B in different frames. :confused:
 
nassboy said:
I've seen in feynman and on the internet a derivation that the force on a negatively charged particle from neutral current carrying wire can be shown to be purely magnetostatic in one frame of reference and purely electrostatic in the other frame of reference using the length contraction. The contracted wire has a net positive charge, and therefore attracts the negatively charged particle.

I've tried to extend this idea to two current carrying wires(the direction of the current the same in both wires)...but it seems that they both would have positive charge and repel when they should attract.

What am I doing wrong?

Nassboy...
You are failing to take into account the Magnetic fields, in particular the DIRECTION of each B field around each wire.This is the same mistake 'meemoe_uk' was making in a previous thread, (except he would never admit it).

Remember the purpose of that exercise is to derive the MAGNETIC FIELD around the wire...

The DIRECTION of that field around each wire DETERMINES the direction of the force (in the lab frame) on a test charge or upon ANOTHER CURRENT A CARRYING WIRE according to the Lorentz force equation (below)...

F = qv X B (for point charges) (B = mag.field; q = test charge with velocity v outside the wire)

F = Integral ( IL X B) ...( for wires) (where L = length of wire, I = current)
(Your link doesn't point that out very well).
Remember these are the forces YOU as the observer sees in the lab frame.

(Actually, the full Lorentz equaton is F = qE + (qv X B)...but the electric field E is zero in the lab frame since the each wire is electrically neutral in labe frame).

And remember its the 'right hand rule' that determine the direction of the force.
See here for a little more: http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/magfor.html

Creator

P.S. the link you cited is not a very great explanation since it arrived at the "magnetic force" (eqn. # 3) in somewhat non traditional form...and without the Lorentz force eqn. you cannot see in which direction that force is acting.

However, you will see that the mag. force eqn. (equation # 3 in your link) is the same as my equation above because the term in the parenthesis is simply equal to B...IOW, simply substitute B = uI / 2(pi)R (Ampere's law) for the term in parenthesis and you will recover Lorentz force equation I gave above.)

see:http://hyperphysics.phy-astr.gsu.edu/HBASE/magnetic/magcur.html
 
Last edited:
nassboy said:
I've seen in feynman and on the internet a derivation that the force on a negatively charged particle from neutral current carrying wire can be shown to be purely magnetostatic in one frame of reference and purely electrostatic in the other frame of reference using the length contraction. The contracted wire has a net positive charge, and therefore attracts the negatively charged particle.

I've tried to extend this idea to two current carrying wires(the direction of the current the same in both wires)...but it seems that they both would have positive charge and repel when they should attract.

What am I doing wrong?
Let's put the same current in each wire so the mean electron drift velocities are equal. Each moving electron in wire 2 sees a net positive charge in wire 1--this is the case that you say Feynman considers--so the electrons are attracted towards the other wire. The positive copper ions in wire 2 are at rest, however. They see an electrically neutral wire 1, and feel no force. The system is symmetric, so everything we said about wire 2 applies also to wire 1. The mutual force is attractive.

Creator: you've missed the point of this thread. The OP's link demonstrates the relativistic unity of electric and magnetic forces.
 
I still don't see why both wires aren't length contracted and therefore have a positive charge...

Only one wire is moving and not both?
 
tiny-tim said:
nassboy said:
I've seen in feynman and on the internet a derivation that the force on a negatively charged particle from neutral current carrying wire can be shown to be purely magnetostatic in one frame of reference and purely electrostatic in the other frame of reference using the length contraction.
Hi nassboy! :smile:

That doesn't look right …

E2 - B2 is invariant (independent of the frame of reference), so you can't have the same field with just E or just B in different frames. :confused:

It is possible that [itex]\boldsymbol{E}=0[/itex] and [itex]\boldsymbol{B}\neq 0[/itex] in some frame, so that a particle feels only a magnetic force, and [itex]\boldsymbol{E}\neq 0[/itex] and [itex]\boldsymbol{B}\neq 0[/itex] and [itex]\boldsymbol{v}=0[/itex] in some other frame, so that a particle feels only an electric force.
 
nassboy said:
I still don't see why both wires aren't length contracted and therefore have a positive charge...

Only one wire is moving and not both?
The wires aren't moving, only the electrons in the wires.
 
  • #10
nassboy said:
I've seen in feynman and on the internet a derivation that the force on a negatively charged particle from neutral current carrying wire can be shown to be purely magnetostatic in one frame of reference and purely electrostatic in the other frame of reference using the length contraction. The contracted wire has a net positive charge, and therefore attracts the negatively charged particle.

I've tried to extend this idea to two current carrying wires(the direction of the current the same in both wires)...but it seems that they both would have positive charge and repel when they should attract.

What am I doing wrong?

If they both have positive charge they should have repulsive electrostatic force. But the attractive magnetic force due to moving proton will be more. Thus the total force on wire will be attractive. U failed to see the magnetic force.
 
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  • #11
lovetruth said:
There is nothing wrong with your understanding. The problem is in the relativity theory and the eroneous derivation by feynmann. I kno i am challenging Feynman and einstein authority but, please read my explanation below for what is wrong in both the theory and derivation. I will only consider the charges(proton and electron) in the wire.
:rolleyes:

So far so good for the magnetostatic case. The real error is done in electrostatic case.

For the electrostatic case,
the proton are at rest so their length is more in this frame than in the magnetostatic frame. The proton density is reduced in the electrostatic case. This increase in length of proton in electrostatic case is ignored in the derivation. The protons length was contracted when the protons were moving in the magnetostatic case. If the protons come at rest in electrostatic frame, they must come to their orignal length which is greater than in magnetostatic frame(in which proton length contraction occur).
electron length will contract and increase electron density(which is correctly shown in the derivation), but proton length expansion is ignored in derivation.
Now u kno the error in derivation.
Even after accounting the error done in derivation, relativity theory gives different result. thus, the theory must be wrong.
Nonsense. Length contraction is most definitely considered.
 

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