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- Thread starter Tracer
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There are still questions.

How is the observed red shift converted to a relative velocity?

Method #1.

Is the value of Fobserved divided by Fsource just plugged into the relativistic Doppler effect equation (RDE) and then solved for RV? Using this method, if Fo/Fs is 0.5773503 then RV will be determined to be 0.5c.

However the Relativistic Doppler effect equation treats RV as being applied to both a classical non-relativistic Doppler effect and a relativistic Doppler effect. This is wrong in this scenario since there should be no relativistic effects between the earth and the distant galaxy since both objects are at rest in their own local space.(except for very small values of peculiar motions of the bodies involved).

Method #2.

The way to determine an RV based on the observed red shift when only separation velocities due to Hubble expansion are involved, should be to use just the classical Doppler effect. Using this approach RV = (1-Fo/Fs)/(Fo/Fs)

which is V = 0.7320507c for Fo/Fs = 0.5773503.

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ghwellsjr

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If R is the Ratio of the two frequencies, then:There are still questions.

How is the observed red shift converted to a relative velocity?

Method #1.

Is the value of Fobserved divided by Fsource just plugged into the relativistic Doppler effect equation (RDE) and then solved for RV? Using this method, if Fo/Fs is 0.5773503 then RV will be determined to be 0.5c.

β = |(1-R

This works for both red and blue shifts and for ratios of time intervals or periods as well as for frequencies, assuming that the motion is in line with the observer.

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Thank you George for your reply. However my question is whether or not β caused by hubble expansion causes relativistic effects. My previous post shows that the value of β will be considerably different if there are relativistic effects and when there are not. Which method is correct?If R is the Ratio of the two frequencies, then:

β = |(1-R^{2})/(1+R^{2})|

This works for both red and blue shifts and for ratios of time intervals or periods as well as for frequencies, assuming that the motion is in line with the observer.

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Note that although the title and the first sentence specify special relativity, the remainder of the thread discusses cosmology where special relativity is not valid and general relativity must be used.What exactly comprises a relative velocity in special relativity? I find it confusing when distant galaxies can be moving away from the earth at speeds approaching the speed of light and yet that separation speed contributes nothing to a relative velocity...

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That is curious. At what RV or distance does SRT become invalid?Note that although the title and the first sentence specify special relativity, the remainder of the thread discusses cosmology where special relativity is not valid and general relativity must be used.

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β = |(1-R2)/(1+R2)|

This works for both red and blue shifts and for ratios of time intervals or periods as well as for frequencies, assuming that the motion is in line with the observer.

I take that as a vote for "hubble expansion causes time dilation". Correct me if that is not what you meant.

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SR is invalid whenever curvature is significant.That is curious. At what RV or distance does SRT become invalid?

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ghwellsjr

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No, that's not what I meant. I simply was showing the equation for the sake of others that you used to do your calculation for method 1 which applies only to Special Relativity. I wasn't answering your question.

β = |(1-R2)/(1+R2)|

This works for both red and blue shifts and for ratios of time intervals or periods as well as for frequencies, assuming that the motion is in line with the observer.

I take that as a vote for "hubble expansion causes time dilation". Correct me if that is not what you meant.

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Does GR consider hubble expansion to be curvature?SR is invalid whenever curvature is significant.

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Hi Tracer: first, it's good when you realize you are confused..... This whole cosmology thing IS very confusing....and still confounds me. [If I get something wrong here, somebody please correct it.] After reading this, you may be sorry you asked about velocity in GR!!(LOL)

As Dalespam notes, your title and question apply to two different regimes, SR and GR, respectively.

Distant galaxies CAN be moving away from the earth at speeds GREATER than the speed of light....and so much, but not all, and probably most, of the universe is way beyond our ability to detect via light.

Wikipedia explains further this way:

and for a simple illustration of the "curve" :

Forgetting increasing spatial separation,expansion of the universe, for a few moments, and expanding on the Wikipedia comments:

In SR, flat spacetime, relative velocities at distant points can be compared. Distances are well defined; In GR, curved spacetime, velocity comparisons can only be made at some common measurement point. Distances are NOT well defined because of curvature; There is no global frame of reference in GR.

[This is what Dalespam explained:

To define a frame (or observer, who has clocks and rulers ) in curved spacetime we must know something about the worldline, the curve (in space and time) along which the frame is carried. This is called parallel transport and different worldlines give different results!!!

I'll stop here because how all this exactly relates to redshift interpretations has been argued in these forums and I am not confident I understand it.

Expansion: I saved this explanation from Chalnoth and Marcus (whom I trust) :

As Dalespam notes, your title and question apply to two different regimes, SR and GR, respectively.

Distant galaxies CAN be moving away from the earth at speeds GREATER than the speed of light....and so much, but not all, and probably most, of the universe is way beyond our ability to detect via light.

Wikipedia explains further this way:

http://en.wikipedia.org/wiki/Metric_expansion_of_space#Measuring_distance_in_a_metric_spaceIn expanding space, distance is a dynamical quantity which changes with time. There are several different ways of defining distance in cosmology, known as distance measures, but the most common is comoving distance.

The metric only defines the distance between nearby points. In order to define the distance between arbitrarily distant points, one must specify both the points and a specific curve connecting them. The distance between the points can then be found by finding the length of this connecting curve.

and for a simple illustration of the "curve" :

from the above source.On the curved surface of the Earth, we can see this effect in long-haul airline flights where the distance between two points is measured based upon a Great circle, and not along the straight line that passes through the Earth. While there is always an effect due to this curvature, at short distances the effect is so small as to be unnoticeable.

Forgetting increasing spatial separation,expansion of the universe, for a few moments, and expanding on the Wikipedia comments:

In SR, flat spacetime, relative velocities at distant points can be compared. Distances are well defined; In GR, curved spacetime, velocity comparisons can only be made at some common measurement point. Distances are NOT well defined because of curvature; There is no global frame of reference in GR.

[This is what Dalespam explained:

In general relativity, an inertial reference frame is only an approximation that applies in a region that is small enough for the curvature of space to be negligible. So space is curved over larger distances but we keep our observations to only a small region for comparisons. Another way to say this: In curved spacetime there's no globally valid transformation between frames as there is in flat spacetime.SR is invalid whenever curvature is significant

To define a frame (or observer, who has clocks and rulers ) in curved spacetime we must know something about the worldline, the curve (in space and time) along which the frame is carried. This is called parallel transport and different worldlines give different results!!!

I'll stop here because how all this exactly relates to redshift interpretations has been argued in these forums and I am not confident I understand it.

Expansion: I saved this explanation from Chalnoth and Marcus (whom I trust) :

I am aware the Hubble constant apparently varies over time....how that affects the above is another issue that confuses me!The simplest way I can think to say it is that you get some very specific total redshift for faraway objects due to the expansion. How much of that redshift is due to the doppler shift and how much is due to the expansion between us and the far away object is completely arbitrary....

the recession velocity is sort of the "obvious" velocity that you would write down: it's simply the Hubble expansion rate times the instantaneous distance to the object (the instantaneous distance is the distance given by the time it would take light rays to traverse the distance if you could instantly freeze the expansion to let those light rays do the bouncing)......

you have a far-away universe emitting light in our direction in the early universe. At the time the light was emitted, the recession velocity of this galaxy was greater than the speed of light, and so as the light moved in our direction, the expansion of our universe carried it away faster than it could approach us.

Redshift vs recession: It's largely just a matter of the description of reality rather than actually being a physical discrepancy. If you so choose, you can select a different coordinate system where the expansion appears to be primarily due to the recession instead of the expansion. The math is just easier in the coordinate system where the expansion is the cause of the redshift.

Marcus: There are several different measures of distance. Recession speed (better called recession rate) is the rate that distance to something is increasing. Before specifying a recession rate one should really say WHICH measure of distance one is using. As Chalnoth pointed out the natural measure when discussing Hubble Law expansion is the instantaneous distance (where you imagine freezing the expansion process at a particular moment so you can measure it, by bouncing a radar signal or however you like, and so measure the distance at that moment). The Hubble Law v = HD is stated in terms of that distance. For the law to apply, D is understood to be the distance "now" (at some moment) and v the current rate that distance is expanding.

If anyone can simplify this, BRAVO!!!However, our universe has an expansion rate (hubble parameter) that is slowing down. So, after some amount of time, after the light ray had traversed some distance, eventually the expansion rate slowed enough that the light ray started to make headway against the expansion, finally reaching us billions of years later. .... So even though the expansion rate slowed enough that the light ray could eventually get to us, it didn't need to slow enough for that galaxy to stop receding at faster than the speed of light...Therefore, there are many galaxies that we can see which always have been and always will be receding at faster than the speed of light.

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Thank you Naty1. Your post helped a lot. I now understand why others have said SRT does not apply.......

To define a frame (or observer, who has clocks and rulers ) in curved spacetime we must know something about the worldline, the curve (in space and time) along which the frame is carried. This is called parallel transport and different worldlines give different results!!!

I'll stop here because how all this exactly relates to redshift interpretations has been argued in these forums and I am not confident I understand it.

Expansion: I saved this explanation from Chalnoth and Marcus (whom I trust) :

I am aware the Hubble constant apparently varies over time....how that affects the above is another issue that confuses me!

If anyone can simplify this, BRAVO!!!

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Yes. Roughly speaking it is curvature in the time dimension.Does GR consider hubble expansion to be curvature?

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