Speed of light in an expanding universe

Warp
Messages
139
Reaction score
15
From answers given to me here and elsewhere, I finally got a (what I think should be the right) answer to the problem:

Suppose that the universe were expanding in such a way that two planets were receding from each other at a constant speed of 1.1c (or, in other words, their distance would grow at a constant speed of 1.1c). Assume that one of the planets sends a light ray to the other. Will the light ray ever reach the other planet?

Quite surprisingly and rather unintuitively, the answer seems to be yes: The light ray does reach the other planet eventually, even though that planet is receding faster than c. The mechanism behind this lies in how the geometry of the universe is changing, and is easiest understood with an analogy: If there's an infinitely stretchable rubber band with a snail on one end, and the snail advances 1 meter per hour and the rubber band is stretched 1.1 meters per hour, will the snail ever reach the other end? The answer is yes.

This got me thinking: The snail reaches the other end because it's effectively traveling faster than 1 m/hour (because the stretching rubber band is "pulling" the snail).

Doesn't it likewise mean that the ray of light is effectively traveling faster than c, or else it would never reach the other planet?

Does this mean that the speed that light effectively travels is larger in an expanding universe than in a (hypothetical) steady-state universe? (And conversely, light would travel slower in a shrinking universe.)

If the answer is yes, then what consequences does this have to the definition of c?
 
Physics news on Phys.org
Warp said:
This got me thinking: The snail reaches the other end because it's effectively traveling faster than 1 m/hour (because the stretching rubber band is "pulling" the snail).

I think an easier way to visualize this is that after the snail has moved 1/10 of the rubber band's length, then the stretching of the rubber band ahead of the snail is smaller than 1m/hour. The snail moves with respect to the rubber band always at 1m/s. Likewise, photon move with respect to space always at the speed c.
 
clamtrox said:
I think an easier way to visualize this is that after the snail has moved 1/10 of the rubber band's length, then the stretching of the rubber band ahead of the snail is smaller than 1m/hour. The snail moves with respect to the rubber band always at 1m/s. Likewise, photon move with respect to space always at the speed c.

But that's why I used the word "effectively". The distance between the two planets grows faster than c, and thus in order for light to be able to catch up with that receding planet, it has to effectively move even faster.

In other words, light is effectively moving faster than c, which kind of sounds like a contradiction (especially since the speed of light in vacuum is supposed to be constant).
 
In GR, the local speed of light in vacuum is c. This is the appropriate generalization of the statement in SR that "the speed of light in vacuum is c." Any "contradictions" come from trying to use an inappropriate generalization.

If you could measure the speed of a light pulse as it whizzes right past you, using measurements confined to a region where spacetime curvature is insignificant, you would always get c. Distance/time for the same light pulse, over a distance large enough for spacetime curvature to be significant, is another matter.
 
Warp said:
But that's why I used the word "effectively". The distance between the two planets grows faster than c, and thus in order for light to be able to catch up with that receding planet, it has to effectively move even faster.

In other words, light is effectively moving faster than c, which kind of sounds like a contradiction (especially since the speed of light in vacuum is supposed to be constant).

Suppose I have point A and point B 1 meter apart. Then I fire a bullet from A to B. While it's moving, I move point A 1 meter backwards. Did I just double the bullet's "effective speed"?

If we return to the snail analogy, I can take a guess of what you are thinking. You are thinking that the snail is on top of the rubber band, and the stretching is making it move faster with respect to the ground. But now when we switch from rubber bands to space, there is nothing physical acting as the "ground" in this analogy. You can of course embed an expanding universe into a static one, and in that case things work exactly like in the snail analogy. But you have no reason to talk about quantities in the static background, because that's just a mathematical trick you've done. It corresponds to nothing physical. Velocities are only meaningful if you define them with respect to the rubber band.
 
Suppose that the universe were expanding in such a way that two planets were receding from each other at a constant speed of 1.1c (or, in other words, their distance would grow at a constant speed of 1.1c). Assume that one of the planets sends a light ray to the other.
How does one calculate the redshift in a case like this?

EDIT: I'll answer my own question. The redshift is λnowthen = anow/athen, where a(t) is the "radius", a length characteristic of the size of the expanding universe. The redshift we observe depends only on how much the radius changes from emission to reception, not how fast it took. So it's independent of da/dt, and having da/dt > c would not be a contradiction.
 
Last edited:
In Philippe G. Ciarlet's book 'An introduction to differential geometry', He gives the integrability conditions of the differential equations like this: $$ \partial_{i} F_{lj}=L^p_{ij} F_{lp},\,\,\,F_{ij}(x_0)=F^0_{ij}. $$ The integrability conditions for the existence of a global solution ##F_{lj}## is: $$ R^i_{jkl}\equiv\partial_k L^i_{jl}-\partial_l L^i_{jk}+L^h_{jl} L^i_{hk}-L^h_{jk} L^i_{hl}=0 $$ Then from the equation: $$\nabla_b e_a= \Gamma^c_{ab} e_c$$ Using cartesian basis ## e_I...
Thread 'Can this experiment break Lorentz symmetry?'
1. The Big Idea: According to Einstein’s relativity, all motion is relative. You can’t tell if you’re moving at a constant velocity without looking outside. But what if there is a universal “rest frame” (like the old idea of the “ether”)? This experiment tries to find out by looking for tiny, directional differences in how objects move inside a sealed box. 2. How It Works: The Two-Stage Process Imagine a perfectly isolated spacecraft (our lab) moving through space at some unknown speed V...
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. The Relativator was sold by (as printed) Atomic Laboratories, Inc. 3086 Claremont Ave, Berkeley 5, California , which seems to be a division of Cenco Instruments (Central Scientific Company)... Source: https://www.physicsforums.com/insights/relativator-circular-slide-rule-simulated-with-desmos/ by @robphy
Back
Top