Length Contraction vs. Distance Contraction

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Discussion Overview

The discussion revolves around the concepts of length contraction and distance contraction as perceived by different observers in the context of special relativity. Participants explore whether these phenomena are distinct or part of the same underlying principle, particularly in relation to the Lorentz transformation. The scope includes theoretical implications and conceptual clarifications regarding how these contractions are observed in different frames of reference.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory

Main Points Raised

  • Some participants propose that length contraction and distance contraction are the same phenomenon as described by the Lorentz transform.
  • Others argue that these contractions occur in different frames, leading to confusion about their equivalence.
  • A participant suggests that in the rest frame, the moving body is contracted, while in the moving frame, the distance to an external point is affected.
  • Another participant illustrates a scenario involving a rod and distances between observers to highlight the complexities of these contractions in different frames.
  • Some contributions emphasize that length contraction only occurs along the direction of motion and not perpendicular to it.
  • There are claims that the effects of time dilation and the relativity of simultaneity complicate the application of the Lorentz transform beyond simple length contraction.
  • Participants note that both observers see different contractions based on their relative motion, leading to differing interpretations of the same scenario.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether length contraction and distance contraction are the same phenomenon. Multiple competing views remain, with some asserting they are equivalent and others maintaining they are distinct due to their dependence on the observer's frame of reference.

Contextual Notes

Limitations include the dependence on definitions of length and distance contraction, as well as unresolved mathematical steps regarding the application of the Lorentz transform in different scenarios.

arindamsinha
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Consider observer A at rest, seeing observer B traveling in a rocket at high speed towards a star C. Star C is at rest w.r.t. A.

A in his frame sees B's rocket to be length contracted. B considers his distance to C to be shorter than (contracted) compared to what A sees.

I seem to be finding the term 'length contraction' being used for describing both phenomena. I feel these are two separate phenomena (though perhaps 2 sides of the same coin) as they are observed in different observers' frames.

Are there separate terms to describe these two contractions (length and distance), or are they considered the same phenomenon?
 
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They are both the same thing, part of the Lorentz transform.
 
DaleSpam said:
They are both the same thing, part of the Lorentz transform.

I am wondering how they can be the same thing. These two are happening in two different frames. In the rest frame, the moving body is affected. In the moving frame, something external (a distance) is affected.

I am not able to understand how they can be the same.

(Understand that they are both Lorentz transformation related, but so are many other aspects like time dilation, which is not the same manifestation of LT as the above phenomena).
 
arindamsinha said:
I am wondering how they can be the same thing. These two are happening in two different frames. In the rest frame, the moving body is affected. In the moving frame, something external (a distance) is affected.

I am not able to understand how they can be the same.

(Understand that they are both Lorentz transformation related, but so are many other aspects like time dilation, which is not the same manifestation of LT as the above phenomena).

Every frame is a rest frame. Picture two lights on the end of a ruler. If it is moving towards you and one light reaches you have have:

- ruler shorter
- light at end of it closer

Same thing, as Dalespam said.
 
arindamsinha said:
I am wondering how they can be the same thing. These two are happening in two different frames. In the rest frame, the moving body is affected. In the moving frame, something external (a distance) is affected.

Suppose that A and C are separated by two light years, as measured in the frame in which both are at rest. B is midway between them, one light year from C. Now let us imagine that there is a rod, a full light year long, sticking out from C towards A. Because B is at the halfway point, he has just reached the end of that rod.

In the frame in which A and C are at rest (you called it "the rest frame", and that's a bad habit) only B is moving and contracted.

In the frame in which B is at rest, A, C, and the rod are all moving, so are contracted. And B is at one end of the rod and C is at the other, so the length of the rod is the distance between B and C. So if the rod is contracted in the frame in which B is at rest, so is the distance to C.
 
arindamsinha said:
(Understand that they are both Lorentz transformation related, but so are many other aspects like time dilation, which is not the same manifestation of LT as the above phenomena).
Length contraction requires two material points at rest wrt each other. Then, according to the Lorentz transform, the distance between them in their mutual rest frame is greater than the distance in any other frame.
 
PAllen said:
Every frame is a rest frame. Picture two lights on the end of a ruler. If it is moving towards you and one light reaches you have have:

- ruler shorter
- light at end of it closer

Same thing, as Dalespam said.

OK. If I understand correctly, the ruler is shorter and light is closer 'in the direction of motion'. In the reverse direction (opposite the motion) ruler is longer and light is farther. Is that a correct interpretation?
 
Nugatory said:
... In the frame in which B is at rest, A, C, and the rod are all moving, so are contracted. And B is at one end of the rod and C is at the other, so the length of the rod is the distance between B and C. So if the rod is contracted in the frame in which B is at rest, so is the distance to C.

Isn't the AB distance now larger than the BC distance according to B's frame?
 
DaleSpam said:
Length contraction requires two material points at rest wrt each other. Then, according to the Lorentz transform, the distance between them in their mutual rest frame is greater than the distance in any other frame.

I think this works for the length of B's rocket but not for the BC distance... there is still length contraction of BC in spite of them not being at rest to one another...
 
  • #10
arindamsinha said:
OK. If I understand correctly, the ruler is shorter and light is closer 'in the direction of motion'. In the reverse direction (opposite the motion) ruler is longer and light is farther. Is that a correct interpretation?

No. Doppler is different for approach and recession. Length and distance contraction are the same.
 
  • #11
But the length/distance contraction only occurs along the direction of motion, not perpendicular to it.
 
  • #12
arindamsinha said:
Isn't the AB distance now larger than the BC distance according to B's frame?

No. Set up a second rod one light year long extending from A towards C, so that the ends of the two rods are touching in the middle where B is. The AB and the CB rods are both moving relative to B so are both contracted; same γ factor.
 
  • #13
arindamsinha said:
OK. If I understand correctly, the ruler is shorter and light is closer 'in the direction of motion'. In the reverse direction (opposite the motion) ruler is longer and light is farther. Is that a correct interpretation?
No, the math of the Lorentz transform is symmetric this way.
 
  • #14
arindamsinha said:
I think this works for the length of B's rocket but not for the BC distance...
Correct, the front and back of B's rocket are at rest in B's frame. A and C are at rest in A's frame. So A measures the rocket length shorter than B does, and B measures the AC distance shorter than A does.

arindamsinha said:
there is still length contraction of BC in spite of them not being at rest to one another...
Well, the Lorentz transform still applies, but as you mentioned earlier, the Lorentz transform includes other effects (time dilation and relativity of simultaneity) as well. In the case of the material points at rest then all of the other effects cancel out and you are left with the simple length contraction formula, but in general they do not. Specifically, since B and C are moving relative to each other, the relativity of simultaneity effects do not cancel so the formula is more complicated than just the length contraction formula.
 
Last edited:
  • #15
From A's point of view, everything at rest in B's frame is Lorentz-contracted in the direction of relative motion.
From B's point of view, everything at rest in A's frame is Lorentz-contracted in the direction of relative motion.

So B sees the A-C distance contracted. A sees B's rocket contracted.
B thinks he gets there sooner because the distance is less. A says he didn't get there sooner, but he thinks he did because his clock was time-dilated.

Edit: Just a note to say that both views are equally valid as long as B keeps traveling at uniform speed. The situation changes when B slows down and comes to a stop at C. But that's another story - see the Twin Paradox.
 
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