Non-Moving Wormhole & Moving Observer: Paradoxes?

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Discussion Overview

The discussion revolves around the implications of a hypothetical non-moving wormhole and its relationship to closed timelike curves (CTCs) as perceived by a moving observer. Participants explore whether the existence of CTCs is dependent on the motion of the wormhole mouths or the observer's speed, delving into theoretical aspects of spacetime geometry and relativistic effects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants propose that if the mouths of a wormhole do not move relative to each other, then paradoxes associated with CTCs may not arise, even for observers moving at relativistic speeds.
  • Others argue that the existence of CTCs is a geometric property of spacetime and is independent of the motion of observers.
  • Clarifications are sought regarding the original claim about wormholes and CTCs, particularly whether it is possible to have a wormhole configuration without CTCs.
  • One participant expresses uncertainty about how to determine the presence of CTCs and mentions using Minkowski diagrams for understanding basic CTC concepts.
  • Another participant emphasizes that the variety of models and metrics that solve the Einstein Field Equation can lead to different conclusions about the presence of CTCs.
  • There is a mention of a specific paper by Morris, Thorne, and Yurtsever that discusses wormholes and CTCs, which one participant intends to review for further understanding.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the relationship between wormhole motion and the existence of CTCs. Multiple competing views remain, particularly regarding the relevance of observers in determining the presence of CTCs.

Contextual Notes

Some participants express limitations in their understanding of the concepts discussed, indicating a range of familiarity with the subject matter. The discussion also highlights the complexity of the relationship between different models of spacetime and their implications for CTCs.

vemvare
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I've recently come across the claim that if the mouths of a hypothetic wormhole don't move in relation to each other, then paradoxes in the form of closed timelike curves cannot be demonstrated to occur, even if an observer moves at relativistic speed relative to them.

Is this true? I want to be able to graph this, but I don't know how to insert the observer itself to see if it can create paradoxes (as opposed to just seeing things as happening in reverse, which is easily demonstrated), rather than it's relativistic timeframe.

(Do ignore the obvious question how the wormhole mouths got to be in different places. )
 
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vemvare said:
I've recently come across the claim that if the mouths of a hypothetic wormhole don't move in relation to each other, then paradoxes in the form of closed timelike curves cannot be demonstrated to occur, even if an observer moves at relativistic speed relative to them.

Several points need clarification here.

1) The discussion of observers is irrelevant. The existence or nonexistence of CTCs in a spacetime has nothing to do with observers.

2) Where did you find this claim? Has it been stated somewhere in exact language?

3) Which of the following are they claiming? (a) It is possible to write down a metric for a spacetime in which there is a wormhole, the mouths don't move, and there are no CTCs. (b) Given a state with a wormhole, it can't be manipulated in order to form CTCs.

Statement 3b would be false: Morris, Thorne, and Yurtsever, "Wormholes, time machines, and the weak energy condition," Phys Rev Lett 61 (1988) 1446 .
 
1. Then how do you see if there is a CTC? I'm a beginner in the field and I've only quite recently understood why the most basic form of CTC's even occur, by drawing lines in Minkowski diagrams. One thing I've even more recently begun to perhaps understand is that relativity seems to be explainable by a wider range of models/metrics, so that observable relativistic effects can be shown to occur, and what happens when/if c is in some way exceeded is depends on the model used.

2. Modern hard-sf trope. Naturally I have no a great ability to distinguish between informed and uninformed claims as I'm not informed myself. As in "reviewed papers", no, not that I know of.

3. I will look at this paper, see if I can make some sense out of it. I'm sorry that I didn't reply earlier, when someone takes the time to reply to my "noobish" question I feel I should. Well, I'm currently studying mechanics, so, I'll get there eventually :)
 
Last edited:
vemvare said:
how do you see if there is a CTC?

Whether or not CTCs are present is a geometric fact about the spacetime. You check it by looking at the geometry, which means looking at the mathematical description of the spacetime.

vemvare said:
relativity seems to be explainable by a wider range of models/metrics

This is not really the right way to state it. What I think you mean is that there are a wide range of models/metrics that are solutions to the Einstein Field Equation, which is the central equation of General Relativity. This is true, and some of those solutions have CTCs in them, others don't. bcrowell's questions #3a and #3b are asking about particular types of solutions.

vemvare said:
what happens when/if c is in some way exceeded

I'm not sure why you bring this in. CTC stands for closed timelike curve; that means an observer can have that curve as his worldline while always moving slower than ##c##.
 

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