Isotropic Observer: Are They Always At Rest?

  • Context: Graduate 
  • Thread starter Thread starter eoghan
  • Start date Start date
  • Tags Tags
    Isotropic Observer
Click For Summary

Discussion Overview

The discussion revolves around the concept of isotropic observers in the context of homogeneous and isotropic spacetimes, particularly focusing on whether these observers are always at rest in a surface of homogeneity. The scope includes theoretical aspects of general relativity and cosmology, with references to FRW (Friedmann-Robertson-Walker) spacetimes.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants suggest that isotropic observers are defined as those who perceive spacetime as isotropic, particularly in the context of FRW spacetimes.
  • Others argue that while observers can be considered "at rest" at a given instant, they can also move along their worldlines, raising questions about what "at rest" means in this context.
  • A participant points out that the term "isotropic observer" may not be commonly understood and seeks clarification on its implications.
  • Some participants clarify that comoving observers remain at the same spatial coordinates in standard FRW coordinates, thus being "at rest" in that chart, but they may not be at rest relative to each other.
  • There is a discussion about the relationship between isotropic observers and measurements of the cosmic microwave background radiation (CMBR), with some suggesting that isotropic observers would measure isotropic CMBR readings.
  • One participant questions the wording of the original post, suggesting it may imply a focus on measurements and the implications of the invariance of the speed of light.
  • Another participant emphasizes that the orthogonality of worldlines to surfaces of homogeneity is an invariant feature of spacetime, independent of the coordinate system used.

Areas of Agreement / Disagreement

Participants express a variety of views on the definitions and implications of isotropic observers, with no clear consensus reached. Some agree on the definitions and implications within the context of FRW spacetimes, while others raise questions and uncertainties about the terminology and concepts involved.

Contextual Notes

Participants note that the meaning of "at rest" requires specification of a reference frame, and the discussion includes various interpretations of isotropic observers and their measurements. There are also references to the complexities introduced by different coordinate systems.

eoghan
Messages
201
Reaction score
7
It is said that in the case of a homogeneous and isotropic spacetime, the surfaces of homogeneity must be orthogonal to the tangents to the world lines of the isotropic observer.
Does this mean that the isotropic observers are always at rest in a surface of homogeneity?
 
Physics news on Phys.org
Sounds like asking; do all observers measure proper time/length?

Is that similar to your question?

Always "at rest"? Always measure time/length properly:smile:; according to how they are defined.

Relative motion is (generally*) not part of measuring time/length, either is "at rest".

*those measurements taken while accelerating causes "issues", but given your choice of words I'd guess you are aware of this point...also.

Oh and is that a common term? "isotropic observer" never heard it before and can't picture what it would "mean".
 
Last edited:
No, it means that a given time the properties of the space are the same everywhere. At a given instant of course an observer is "at rest", but then it can move along its worldline!
 
oh yea isotropic is pretty commonly understood, especially in a physics forum. "Isotropic observer", given the definitions of "observer" & isotropic from a physics perspective, left me unsure if something besides plain ol' "observer" was implied.

I tried adding the definitions together...and it didn't add up.

"At a given instant of course an observer is "at rest"," :confused: relative to what?? the way time/length is measured?

anyhoo let's not carry on with this.
 
eoghan said:
It is said that in the case of a homogeneous and isotropic spacetime, the surfaces of homogeneity must be orthogonal to the tangents to the world lines of the isotropic observer.

If by "isotropic observer" you mean "an observer that sees the spacetime as isotropic", then yes, this is true. At least, it's true of the standard example of a homogeneous and isotropic spacetime, FRW spacetime.

eoghan said:
Does this mean that the isotropic observers are always at rest in a surface of homogeneity?

Yes. This is a bit of a strange way of stating it, though; the more standard way of stating it requires you to first set up the standard FRW coordinate chart, and then observe that what you are calling isotropic observers (the more usual term is "comoving" observers) remain at the same spatial coordinates in this chart for all time, hence are "at rest" in this chart.

It's also good to bear in mind that these comoving observers, although they are "at rest" in the standard coordinate chart, are *not* "at rest" relative to each other in other senses in an FRW spacetime. For example, if two comoving observers exchange light signals, they will see the round-trip travel times of the light signals continually increase or decrease (depending on whether they are in an expanding FRW spacetime or a contracting one).
 
PeterDonis said:
If by "isotropic observer" you mean "an observer that sees the spacetime as isotropic", then yes, this is true. At least, it's true of the standard example of a homogeneous and isotropic spacetime, FRW spacetime.



Yes. This is a bit of a strange way of stating it, though; the more standard way of stating it requires you to first set up the standard FRW coordinate chart, and then observe that what you are calling isotropic observers (the more usual term is "comoving" observers) remain at the same spatial coordinates in this chart for all time, hence are "at rest" in this chart.

It's also good to bear in mind that these comoving observers, although they are "at rest" in the standard coordinate chart, are *not* "at rest" relative to each other in other senses in an FRW spacetime. For example, if two comoving observers exchange light signals, they will see the round-trip travel times of the light signals continually increase or decrease (depending on whether they are in an expanding FRW spacetime or a contracting one).
From this it seems "isotropic " observer means measuring isotropic CMBR readings , is this right?
 
Austin0 said:
From this it seems "isotropic " observer means measuring isotropic CMBR readings , is this right?

In a universe with a CMBR, such as ours, yes. More generally, whatever matter/energy/radiation is present will appear isotropic to an "isotropic observer". (Obviously this only holds approximately in our actual universe.)
 
nitsuj said:
oh yea isotropic is pretty commonly understood, especially in a physics forum. "Isotropic observer", given the definitions of "observer" & isotropic from a physics perspective, left me unsure if something besides plain ol' "observer" was implied.

I tried adding the definitions together...and it didn't add up.
I've read it in "Wald - General Relativity". It means an observer who sees the universe as isotropic.



alialice said:
At a given instant of course an observer is "at rest", but then it can move along its worldline!
The problem is that the worldline is always orthogonal, so the observer will always be at rest relative to the surface of homogeneity


PeterDonis said:
Yes. This is a bit of a strange way of stating it, though; the more standard way of stating it requires you to first set up the standard FRW coordinate chart, and then observe that what you are calling isotropic observers (the more usual term is "comoving" observers) remain at the same spatial coordinates in this chart for all time, hence are "at rest" in this chart.
Uhm.. if I take a picture of the universe at a frozen time t, then that is a surface of hoogeneity, is it right?
 
eoghan said:
I've read it in "Wald - General Relativity". It means an observer who sees the universe as isotropic.




The problem is that the worldline is always orthogonal, so the observer will always be at rest relative to the surface of homogeneity



Uhm.. if I take a picture of the universe at a frozen time t, then that is a surface of hoogeneity, is it right?

I find the question as worded in the OP kind of awkward.

Personally I see it as asking about measurements, and the "consequence/effect" the invariance of c has on those measurements.

"The problem is that the worldline is always orthogonal, so the observer will always be at rest relative to the surface of homogeneity"

Like Peter said this is "coordinates".

As stated above I can't help but feel the train of thought would continue to "at rest" we are traveling at c relative to..., or some other similar "Greene" interpretation.
 
  • #10
eoghan said:
Uhm.. if I take a picture of the universe at a frozen time t, then that is a surface of hoogeneity, is it right?

If the time "t" is the time in the standard FRW chart (which is the same as proper time for "comoving" observers), then yes.
 
  • #11
nitsuj said:
Personally I see it as asking about measurements, and the "consequence/effect" the invariance of c has on those measurements.

The reference to Wald makes it clear that the OP is talking about FRW spacetimes and their properties. I don't think the OP meant to raise any issues about measurements, the invariance of c, etc. (though he can of course correct me if I'm wrong).

nitsuj said:
Like Peter said this is "coordinates".

I did say that, but now I need to clarify that it's not *just* coordinates. :redface:

For the term "at rest" to be meaningful, one has to specify "at rest relative to what?" The standard FRW coordinate chart uses the worldlines of comoving observers as the standard of "rest"; each comoving worldline stays at the same spatial coordinates for all time. But the comoving worldlines themselves are invariant features of the spacetime; you can describe them in any coordinate chart you like, they just won't look as simple in any chart other than the standard FRW chart.

Similarly, the fact that the worldlines of comoving observers are orthogonal to the surfaces of homogeneity is an invariant; it does not depend on the coordinate chart. It's just easiest to illustrate this fact in the standard FRW chart, since the surfaces of homogeneity are just surfaces of constant time in this chart.

Sorry if the above wasn't clear from my previous posts.
 
  • #12
Opps, then it's my mistake Peter.

I don't even know what FRW is.

Sorry 'bout confusing the thread.
 
  • #14
PeterDonis said:
If the time "t" is the time in the standard FRW chart (which is the same as proper time for "comoving" observers), then yes.

So if I am an isotropic observer (then "t" is the time in the standard FRW) I must be at rest in a given surface of homogeneity, can't I move?
 
  • #15
eoghan said:
So if I am an isotropic observer (then "t" is the time in the standard FRW) I must be at rest in a given surface of homogeneity, can't I move?

Of course you "can" move (meaning you can have a worldline that does not stay at the same spatial coordinates for all time in the standard FRW chart). But if you move, you won't be an isotropic observer any more--you won't see the universe as being the same in all directions.
 
  • #16
eoghan said:
Uhm.. if I take a picture of the universe at a frozen time t, then that is a surface of hoogeneity, is it right?

On re-reading this, I realized I should comment on the phrase "take a picture". I was interpreting that to mean "take a particular spacelike slice of constant FRW coordinate time t out of the entire spacetime". Any such spacelike slice is a surface of homogeneity.

However, if you were to literally "take a picture" of the light rays entering your eyes (or your camera's lens) at a particular instant, in a standard FRW spacetime, what would be in the picture would *not* be the same as what is in a spacelike slice. What is in the picture, taken literally, would be what is present on your past light cone at the instant at which the picture is taken. And that will *not* be homogeneous (though it will still be isotropic), because the light coming to you at a given instant was emitted at different times, depending on how far away the objects emitting it are.
 
  • #17
Thank you all for the answers. I've understood the whole thing (I think)
 

Similar threads

  • · Replies 16 ·
Replies
16
Views
2K
  • · Replies 51 ·
2
Replies
51
Views
4K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 24 ·
Replies
24
Views
3K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 29 ·
Replies
29
Views
926
  • · Replies 9 ·
Replies
9
Views
2K