Simultaneity in Non-Observable Universe: Is it Possible?

Click For Summary

Discussion Overview

The discussion revolves around the concept of simultaneity in the context of events that are beyond the observable universe. Participants explore whether it is possible to determine simultaneity for such distant events and the implications of relativity on this notion.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants propose that simultaneity can be defined using co-moving coordinates, suggesting that events can be considered simultaneous if they occur at the same time according to co-moving observers after the Big Bang.
  • Others argue that events in the non-observable universe cannot be classified as being in our past or future since their information cannot reach us, raising questions about the nature of simultaneity in such contexts.
  • A participant expresses confusion regarding the measurements of distant co-moving observers, indicating a belief that one must be able to observe their clocks to determine simultaneity.
  • Another viewpoint suggests that while one cannot know what has happened until it is observed, hypothetical discussions about events happening in the non-observable universe are still possible, emphasizing the need to define "now" in relativity.
  • Some participants note that general relativity encompasses all spacetime geometries, which may allow for the adoption of simultaneity conventions that include events outside the observable universe, though these conventions cannot be connected to physical observations.
  • There is a discussion about the limitations of Minkowski space in accounting for cosmic expansion, with some suggesting that simultaneity can be defined in cosmology in ways that are not possible in special relativity.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the nature of simultaneity for events beyond the observable universe. Multiple competing views remain regarding how simultaneity can be defined and the implications of relativity.

Contextual Notes

Limitations include the dependence on definitions of simultaneity and the challenges posed by the inability to communicate with events beyond the observable universe. The discussion also highlights the differences between special and general relativity in defining simultaneity.

Chris Miller
Messages
371
Reaction score
35
Is there any method/model for determining simultaneity of events farther apart than light can ever travel? I'm guessing not. Would it be wrong to say that the non-observable universe exists only in our past (or future)?
 
Physics news on Phys.org
You can adopt any simultaneity convention you like. Typically people use co-moving coordinates as "the" time, in which case one can define simultaneous as meaning two events which occur the same time (as determined by a co-moving observer) after the big bang singularity. Or that occurred when the temperature of the CMB (measured by co-moving observers at each event) was the same.
 
Chris Miller said:
Would it be wrong to say that the non-observable universe exists only in our past (or future)?
My understanding of light cones tells me events in the non-observable universe are not in our past or future, since their information cannot reach us.
 
Last edited:
Thanks Ibix. Problem for me here is that I have no idea what my distant co-moving observer's measurements are, was under the impression that I had to be able to "see" her clock through some hypothetically super-powerful telescope and then subtract the light travel time to know, say, that my 2018: Jan 1: 00:00:00 is her 2035: Mar 6: 13:30:05. Or whatever.

I share your confusion here stoomart. Practically speaking, simultaneity beyond light's reach seems undefined.
 
You don't know what's happened until you see it, no. And my understanding is that there are parts of the universe you'll never see. But you can talk hypothetically about what's happening now somewhere you can't see (or won't see until later). The only extra wrinkle relativity introduces is a requirement to define what you mean by "now" before you do.

Saying simultaneity is undefined where you can't see is a bit like saying the back of your head is undefined because you aren't sitting between a pair of mirrors. I suppose it's possible that the back of my head doesn't exist at the moment, but if so it's strange how it comes into existence the instant someone comes into the room behind me.
 
  • Like
Likes   Reactions: stoomart
Ibix said:
You don't know what's happened until you see it, no. And my understanding is that there are parts of the universe you'll never see. But you can talk hypothetically about what's happening now somewhere you can't see (or won't see until later). The only extra wrinkle relativity introduces is a requirement to define what you mean by "now" before you do.

Saying simultaneity is undefined where you can't see is a bit like saying the back of your head is undefined because you aren't sitting between a pair of mirrors. I suppose it's possible that the back of my head doesn't exist at the moment, but if so it's strange how it comes into existence the instant someone comes into the room behind me.
I understand relativity doesn't apply to Hubble expansion where even though co-moving objects are separating at >c, their light clocks would each appear (if they could each be seen by the other) to run at the same speed. Also Minkowski space doesn't factor in expansion. So maybe this was the wrong forum for my question. I suppose your analogy is valid, although I have seen the back of my head and can examine it in ways other than visually.
 
Chris Miller said:
So maybe this was the wrong forum for my question.

General relativity covers all spacetime geometries, not just Minkowski spacetime. So this is the right forum.

Another way of phrasing the answer you are getting to the original question of this thread is that you can always adopt a simultaneity convention that includes events outside your observable universe. But you won't be able to connect that convention to any physical observation that you can actually make involving those events, the way you can, for example, connect the standard simultaneity convention for inertial frames in flat spacetime to the Einstein clock synchronization procedure.
 
Chris Miller said:
I understand relativity doesn't apply to Hubble expansion where even though co-moving objects are separating at >c, their light clocks would each appear (if they could each be seen by the other) to run at the same speed. Also Minkowski space doesn't factor in expansion. So maybe this was the wrong forum for my question.
In cosmology there's an identifiable "time zero", the Big Bang singularity. And there's an identifiable way to define "two people in the 'same' state of motion", by finding when the CMB is isotropic. Neither of these things can be done in special relativity because the singularity and the CMB don't exist in that case. So you can actually define simultaneity in this case without communication where you can't in special relativity.

You can't actually do anything with the simultaneity convention because you can't communicate. But "at the same time" can be defined perfectly well.
Chris Miller said:
I suppose your analogy is valid, although I have seen the back of my head and can examine it in ways other than visually.
It's not my best analogy.
 

Similar threads

  • · Replies 51 ·
2
Replies
51
Views
5K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 20 ·
Replies
20
Views
3K
  • · Replies 58 ·
2
Replies
58
Views
6K
  • · Replies 9 ·
Replies
9
Views
817
  • · Replies 35 ·
2
Replies
35
Views
4K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 29 ·
Replies
29
Views
4K
  • · Replies 8 ·
Replies
8
Views
1K
  • · Replies 14 ·
Replies
14
Views
1K