Can Relative Velocities Exceed the Speed of Light?

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Discussion Overview

The discussion centers on the concept of relative velocities in the context of special relativity (SR) and general relativity (GR), specifically addressing whether velocities can exceed the speed of light (c) when observed from different reference frames. The scope includes theoretical considerations and mathematical reasoning related to relativistic velocity addition.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant questions how relative velocities can appear to exceed c when multiple observers measure speeds in a linear arrangement, suggesting that observer 4 could be moving away from observer 1 at 1 1/2 c.
  • Another participant responds by explaining the relativistic velocity addition formula, demonstrating that velocities do not add linearly as in classical physics, and provides calculations to illustrate how observer 1 would measure the speed of observer 4 as less than c.
  • The explanation includes references to the effects of length contraction, time dilation, and the relativity of simultaneity, which affect how different observers perceive measurements of distance and time.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the initial question posed, but there is agreement on the application of the relativistic velocity addition formula as a means to resolve the apparent contradiction regarding speeds exceeding c.

Contextual Notes

The discussion relies on the assumptions of special relativity and does not address potential limitations or alternative interpretations of the relativistic framework.

Who May Find This Useful

This discussion may be useful for individuals interested in the principles of special relativity, particularly those exploring the implications of relative motion and velocity measurements in different reference frames.

cbd1
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This is a quite simple question, and hopefully a simple answer. I know the basics of SR and GR, but I'm bothered by this one. It seems that by adding speeds you can get speeds greater than c.

Say we have 4 observers on 4 different bodies. Each observer believes his body to be a rest. We will say that all observers line up to form a straight line progressing from observer 1 -> 4.

Observer 1 views observer 2's body to be moving away at 1/2 c. Oberserver 2 views observer 3 to be moving away at 1/2 c. And observer 3 sees observer 4 to be moving away at 1/2 c. This would mean that observer 4 was moving away from observer 1 at 1 1/2 c. How is the universal maximum c not broken here?
 
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cbd1 said:
This is a quite simple question, and hopefully a simple answer. I know the basics of SR and GR, but I'm bothered by this one. It seems that by adding speeds you can get speeds greater than c.

Say we have 4 observers on 4 different bodies. Each observer believes his body to be a rest. We will say that all observers line up to form a straight line progressing from observer 1 -> 4.

Observer 1 views observer 2's body to be moving away at 1/2 c. Oberserver 2 views observer 3 to be moving away at 1/2 c. And observer 3 sees observer 4 to be moving away at 1/2 c. This would mean that observer 4 was moving away from observer 1 at 1 1/2 c. How is the universal maximum c not broken here?
According to the Lorentz transformation velocities don't add in the way they do in classical physics, instead you have to use the relativistic velocity addition formula. For example, if observer 2 sees observer 3 moving at 0.5c, and observer 1 sees observer 2 moving at 0.5c in the same direction, then observer 1 will see observer 3 moving at (0.5c + 0.5c)/(1 + 0.5*0.5) = 1c/1.25 = 0.8c. Then if observer 3 sees observer 4 moving at 0.5c and observer 1 sees observer 3 moving at 0.8c, that means observer 1 sees observer 4 moving at (0.5c + 0.8c)/(1 + 0.5*0.8) = 1.3c/1.4 = 0.93c.

The fact that velocities don't add in the same way as they do in classical physics has to do with the fact that each observer measures velocity in terms of distance/time on a set of rulers and synchronized clocks at rest relative to themselves, but each observer sees the measurements of rulers and clocks of other observers distorted by length contraction, time dilation, and the relativity of simultaneity (which says that clocks synchronized in one frame will be out-of-sync in other frames).
 
Thanks Jesse for the quick response. That makes sense to me, I think I actually knew that at one time and forgot it. I hate when that happens. I don't use this stuff in my field so it fades out of memory fast.
 

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