Length contraction test in electrical circuits

In summary: during the transient, the length of the wire is greater in an electron frame than in the lab frame, so the moving line of electrons appears length contracted while the static line of atoms in the wire does not?
  • #1
exmarine
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As I am sure everyone is aware, there are still folks who don’t believe SRT and GRT. While 99.9% of them are nut-jobs, there is at least one that I respect – Tom Phipps specifically. I am not familiar with any of his writing before the advent of the GPS satellites. In any case, he now accepts “time dilation”, but not “length contraction”. The last I knew (~2006?) he claimed that it has never been proven empirically. I think he is wrong, and the most compelling evidence of length contraction for me is the explanation of magnetism / Ampere’s law given by Purcell. I assume that at least some of you are familiar with that? Briefly, the apparent length contraction of a passing line of charges enhances their influence on neighboring lines of charges. Thus “parallel currents attract”, i.e., Ampere’s law and magnetism, is so simply and elegantly understood as length contraction, or at least the apparent contraction of a line of charges.

Finally getting to my question: The only objection to Purcell’s interpretation that I can think of is the excess negative charge on a current carrying wire (in the lab frame) that should appear during the starting transient. Since all practical circuits are grounded, I don’t suppose that such would be apparent. But can anyone think of a way to test that – does an excess negative charge appear on a current carrying wire during the starting transient? Or has someone already tested that?

Thanks.
 
  • #3
Physicist J.S Bell thinks that a passing line of objects is not length-contracted.
A relevant line from this page: http://en.wikipedia.org/wiki/Bell's_spaceship_paradox
"The distance between the spaceships does not undergo Lorentz contraction with respect to the distance at the start"

On the other hand Purcell and other people think that a moving capacitor is length-contracted, and charge density is therefore increased.
http://en.wikipedia.org/wiki/Relativistic_electromagnetism

If we measure the current from a circuit to the ground, when a current is started in the circuit, we will notice that there is no current. I mean circuits don't become negatively charged when current is turned on.

Magnetism may be some kind of proof of contraction. People who understand how Lorentz-contraction explains magnetism understand the proof, the problem is that it's difficult to understand.
 
  • #4
jartsa said:
Physicist J.S Bell thinks that a passing line of objects is not length-contracted.
A relevant line from this page: http://en.wikipedia.org/wiki/Bell's_spaceship_paradox
"The distance between the spaceships does not undergo Lorentz contraction with respect to the distance at the start"

On the other hand Purcell and other people think that a moving capacitor is length-contracted, and charge density is therefore increased.
http://en.wikipedia.org/wiki/Relativistic_electromagnetism

If we measure the current from a circuit to the ground, when a current is started in the circuit, we will notice that there is no current. I mean circuits don't become negatively charged when current is turned on.

Magnetism may be some kind of proof of contraction. People who understand how Lorentz-contraction explains magnetism understand the proof, the problem is that it's difficult to understand.
This misunderstands Bell, as well as the scenario Bell analyzed. In that scenario, by construction, the distance remains constant in the starting inertial frame. This is primarily because the accelerations start simultaneously in this frame. In the frame of one of the rockets, the accelerations do not start at the same time, and the distance between the rockets increases.

For a current loop, there are no accelerations (once equilibrium is reached). There are just two different inertial frames to compare. Bell would not dispute that if the distance between electrons in the frame comoving with them is L, then it is less than L in the frame in which the wire is at rest.
 
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  • #5
PAllen said:
For a current loop, there are no accelerations (once equilibrium is reached). There are just two different inertial frames to compare. Bell would not dispute that if the distance between electrons in the frame comoving with them is L, then it is less than L in the frame in which the wire is at rest.
I agree with this. Now the op was precisely about the transient, i.e. the period when the electrons are accelerated as the potential applied between the ends of the wire is increased from 0 to its stationary value (assuming the wire itself is at rest in the lab frame). This does seem similar to the spaceship situation, in the lab frame all electrons simultaneously undergo the same acceleration, and they move apart in their own frames. At the end of the transient the length of the wire is greater in an electron frame than in the lab frame, so the moving line of electrons appears length contracted while the static line of atoms in the wire does not (as with the spaceships, the lab distance between electrons remains the same, it is length contracted relative only to their own frame).
Is this correct ?
 
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  • #6
wabbit said:
I agree with this. Now the op was precisely about the transient, i.e. the period when the electrons are accelerated as the potential applied between the ends of the wire is increased from 0 to its stationary value (assuming the wire itself is at rest in the lab frame). This does seem similar to the spaceship situation, in the lab frame all electrons simultaneously undergo the same acceleration, and they move apart in their own frames. At the end of the transient the length of the wire is greater in an electron frame than in the lab frame, so the moving line of electrons appears length contracted while the static line of atoms in the wire does not (as with the spaceships, the lab distance between electrons remains the same, it is length contracted relative only to their own frame).
Is this correct ?
Transients in wires treated relativistically is surprisingly complex. I was not addressing this case. I looked for some reasonable write up on this available on the web and couldn't find one worth linking to. There have been several involved discussions over the years on this here on PF.
 
  • #7
Thanks. There must also be something wrong in my analysis above since the electrons are always moving very slowly in the wire so relativistic effects can't really be of any significance.
 
  • #8
wabbit said:
At the end of the transient the length of the wire is greater in an electron frame than in the lab frame,

Electron sees an accelerating wire, so electron sees a shortening wire.

As electron sees an expanding line of electrons and a shortening wire, electron concludes that electrons are spouting out of the end of the wire at high speed, if the wire is a straight wire.

If the wire is a loop, it's the same thing, except that electrons stay inside the wire.
 
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  • #9
PAllen said:
This misunderstands Bell, as well as the scenario Bell analyzed. In that scenario, by construction, the distance remains constant in the starting inertial frame. This is primarily because the accelerations start simultaneously in this frame. In the frame of one of the rockets, the accelerations do not start at the same time, and the distance between the rockets increases.

For a current loop, there are no accelerations (once equilibrium is reached). There are just two different inertial frames to compare. Bell would not dispute that if the distance between electrons in the frame comoving with them is L, then it is less than L in the frame in which the wire is at rest.

So in the frame where acceleration of spaceships is simultaneous, spaceship density, number of spaceships per meter, is constant. If spaceships are charged, charge density is constant.

While in the frame of spaceships the spaceship density decreases. If spaceships are charged, charge density is decreases.
 
  • #10
PAllen said:
Transients in wires treated relativistically is surprisingly complex. I was not addressing this case. I looked for some reasonable write up on this available on the web and couldn't find one worth linking to. There have been several involved discussions over the years on this here on PF.

I've missed the arguments / posts on this topic, apparently, but I think it's reasonable to point out to the OP that charge is conserved, so that any buildup of negative charge in one area will have a buildup of positive charge in another.

Additionally, while a full computation of transients in wires would be messy, a computation of what happens in a transmission line is very simple. I'm not feeling motivated to do such a treatment but I'd encourage the OP to look into it giving that they are trying to get a better understanding.

I'd also like to point out that conceptually it's better to think about testing the full Lorentz transform, rather than trying to chop it up into "time dilation" and "length contraction" and the often-neglected (by people who insist on chopping the transform into pieces) effect called "the relativity of simultaneity". If you believe that the whole transform "works", arguments based on chopping it up into pieces seem incoherent.

I believe I've already seen a proof on PF that shows that 3 key experiments experimentally determine all four possible coefficients of a general linear transform between frames, but I couldn't track the link down.

Other arguments (such as the homogeneity and isotropy) rule out nonlinear transforms, as first pointed out by Einstein. This may be a bit abstract, on the experimental side I'd like to point out that that fact that sine-waves in one frame transform to sine-waves in another frame (i.e. no effects of frequency doubling of light or electromagnetic radiation) rule out nonlinear transforms.
 
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  • #11
jartsa said:
Electron sees an accelerating wire, so electron sees a shortening wire.
Yes you re right I misspoke, I was thinking of an "abstract wire" comoving with the electrons here. That one is longer in the electron frame than the physical wire, which is consistent with how you describe it.

Still these effects are truly tiny given the very low velocities concerned, I don't see how they could explain magnetism.
 
  • #13
pervect said:
I'd also like to point out that conceptually it's better to think about testing the full Lorentz transform, rather than trying to chop it up into "time dilation" and "length contraction" and the often-neglected (by people who insist on chopping the transform into pieces) effect called "the relativity of simultaneity". If you believe that the whole transform "works", arguments based on chopping it up into pieces seem incoherent.

Agree. I think it needs saying.
 

1. What is length contraction in electrical circuits?

Length contraction in electrical circuits is a phenomenon in which the length of a moving conductor appears to decrease from the perspective of an observer who is stationary relative to the conductor. This is due to the effects of relativity and can be observed in high-speed circuits.

2. How is length contraction in electrical circuits tested?

Length contraction in electrical circuits can be tested by measuring the length of a conductor at rest and then measuring the length of the same conductor when it is moving at high speeds. The difference in length between the two measurements will indicate the degree of length contraction.

3. What causes length contraction in electrical circuits?

Length contraction in electrical circuits is caused by the Lorentz transformation, which is a mathematical formula that accounts for the effects of relativity on length measurements. This formula shows that as an object approaches the speed of light, its length will appear to decrease from the perspective of a stationary observer.

4. Is length contraction in electrical circuits significant in everyday applications?

In most everyday applications, the speeds at which electrical circuits operate are not high enough to cause noticeable length contraction. However, in high-speed applications such as particle accelerators, length contraction can have a significant impact and must be taken into account in design and calculations.

5. Are there any practical applications of length contraction in electrical circuits?

While length contraction in electrical circuits may not have a direct practical application, it is an important concept to understand in the field of physics and can help explain phenomena such as the behavior of high-speed particles. It also serves as a reminder of the effects of relativity on our perception of the physical world.

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