Speed of Light Paradox: What Did I Miss?

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Discussion Overview

The discussion centers around the measurement of the speed of light by two observers, one stationary and one moving, and the implications of special relativity on their measurements. Participants explore concepts such as time dilation, length contraction, and the relativity of simultaneity, while questioning the assumptions made in the analysis of light propagation in different reference frames.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Observer B measures the speed of light using a tube of proper length L0, while observer A accounts for length contraction and time dilation, leading to a perceived discrepancy in their measurements.
  • Some participants suggest that the relativity of simultaneity is a crucial factor that was not considered in the initial analysis.
  • It is noted that the light's speed remains constant at c in both frames, but the distance traveled by light is affected by the motion of the tube as seen by observer A.
  • Participants discuss how the motion of the tube affects the time it takes for light to travel between the extremities, emphasizing that the distance light travels is not simply the contracted length.
  • One participant proposes a mathematical analysis to show that the distance traveled by light must account for both the length of the tube and the motion of the tube itself.
  • There is a debate over whether the derived equations lead to contradictions regarding the speed of light, with some asserting that the speed remains c while others suggest it appears to change due to relative motion.
  • The concept of a light 4-vector is introduced, discussing how Lorentz transformations maintain the invariance of the speed of light while affecting frequency and wave-number.

Areas of Agreement / Disagreement

Participants express differing views on the implications of special relativity for the measurements of light speed, with no consensus reached on the interpretation of the results or the validity of the initial analysis. The discussion remains unresolved regarding the relationship between the motion of the tube and the propagation of light.

Contextual Notes

Limitations include assumptions about simultaneity and the treatment of distances in different reference frames, as well as unresolved mathematical steps in the derivations presented.

  • #31
"bgq
Posts: 59
YES!
I think I got it!
Let t1 be the time from E to F, and t2 from F to E as measured by A.
According to Lorentz transformation:
t1 = γ(T0/2 + vL0/c2)
t2 = γ(T0/2 - vL0/c2)
d = (L0/γ + vt1) + (L0/γ - vt2)
= 2L0/γ + v(t2 - t2)
= 2L0/γ + v(2γvL0/c2)
= 2L0/γ + 2γL0v2/c2
= 2L0(1/γ + γv2/c2)

so then solving, d = gamma * 2Lo, not divided by gamma as orginally posted,
this confuses me, any explanations would be helpful, thanks
 
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  • #32
randyu said:
[..]
Let t1 be the time from E to F, and t2 from F to E as measured by A.
According to Lorentz transformation:
t1 = γ(T0/2 + vL0/c2)
t2 = γ(T0/2 - vL0/c2)
d = (L0/γ + vt1) + (L0/γ - vt2)
= 2L0/γ + v(t2 - t2)
= 2L0/γ + v(2γvL0/c2)
= 2L0/γ + 2γL0v2/c2
= 2L0(1/γ + γv2/c2)

so then solving, d = gamma * 2Lo, not divided by gamma as orginally posted,
this confuses me, any explanations would be helpful, thanks
Welcome to physicsforums. :smile:

You referred to post #28.

How did you get from
d= 2L0(1/γ + γv2/c2)
to
d = γ * 2Lo ?

Perhaps you did not look at it carefully.
(1/γ + γv2/c2) = 1/γ(1 + γ2v2/c2) ≠ γ
[EDIT: I was wrong, see next]
 
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  • #33
hi harrlylin,

Y=1/sqt(1-v2/c2) > v2/c2=(Y2-1)/Y2
then,
d=2Lo * 1/Y+Y(Y2-1)/Y2= 2Lo*Y
is this not right, thanks
 
  • #34
randyu said:
hi harrlylin,

Y=1/sqt(1-v2/c2) > v2/c2=(Y2-1)/Y2
then,
d=2Lo * 1/Y+Y(Y2-1)/Y2= 2Lo*Y
is this not right, thanks
Oops - I must admit that I did not check bqq's derivation. :blushing:
And yes you are right. Regretfully I did not follow that conversation, [STRIKE]and I won't look into that now. Maybe someone else will, or I will later. [/STRIKE]
What I can say already, is that I see nowhere claimed that d= 2L0/Y :-p

Oh OK I see it: the answer is in post #22. Did you read that?

d is the path length that the light ray travels, and as d>2Lo I suppose that it is the path length in the rest system, with respect to which the apparatus is moving. Do you follow that?

It's like the Michelson-Morley experiment. And it is very well explained in post #17.
So, to elaborate: You walk from the rear of the car to the front of the car and back. As seen from the train tracks, the distance is greater.
- http://en.wikipedia.org/wiki/Michelson–Morley_experiment
 
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  • #35
bgq said:
Hi, there is something I can't understand:

Consider a stationary observer at A. Now consider an observer B in a train that moves with constant velocity v with respect to A. In the train, B tries to measure the speed of light using an empty tube of length L0 (proper length as measured by B). He sends a light signal at extremity E, the signal reaches extremity F (where a mirror exists) and return back to the extremity E. B measure this duration T0 (proper period as measured by B).

Now B measure the speed of light as:

CB = 2L0/T0

Now according to A the length of the tube is contracted and the time is dilated, so he measure the speed of light as:

CA = 2L/T = (2L0/γ)/(γT0) = (L0/T0)/(γ^2) = CB/(γ^2)

which is different from the value measure by B (divided by Gamma squared)

thanks harrylin, what I was thinking is from post #1, d=2Lo/Y and t=YTo which gave c as "divided by gamma squared".
This was wrong from the beginning, the length in the stationary frame is longer than the moving length Lo as you state, confusing because each is moving relative to the other. And also the time is YTo in the "stationary" frame, longer.
I guess this all makes sense, I just get confused about time dilation/expansion using t in different ways it seems to me, sometime an interval, sometimes ticks. Oh well, will come together sooner or later.
Thanks.
 
  • #36
randyu said:
thanks harrylin, what I was thinking is from post #1, d=2Lo/Y and t=YTo which gave c as "divided by gamma squared".
This was wrong from the beginning, the length in the stationary frame is longer than the moving length Lo as you state, confusing because each is moving relative to the other. And also the time is YTo in the "stationary" frame, longer.
I guess this all makes sense, I just get confused about time dilation/expansion using t in different ways it seems to me, sometime an interval, sometimes ticks. Oh well, will come together sooner or later.
Thanks.
That's why it is necessary to make sketches. :-p
Cheers
 

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