Why Does ds^2 Equal 0 in Metrics?

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Discussion Overview

The discussion revolves around the condition ##ds^2=0## in various metrics, particularly in the context of light-like curves in the FLRW and Minkowski metrics. Participants explore the implications of this condition for the speed of light and the nature of light's path in spacetime, addressing both theoretical and conceptual aspects.

Discussion Character

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

Main Points Raised

  • Some participants assert that ##ds^2=0## corresponds to light-like curves, which is a coordinate-independent statement true for any coordinate system.
  • Others argue that in the FLRW metric, the assumption of ##ds^2=0## is related to the computation of redshift for light, emphasizing the use of light-like geodesics.
  • It is noted that for light, ##ds^2=0## is a specific statement about its path, while for massive objects, ##ds^2<0##, and for hypothetical tachyons, ##ds^2>0##.
  • Some participants highlight that the sign convention for metrics affects the interpretation of ##ds^2## for time-like world lines, with different preferences among mathematicians and physicists.
  • A later reply questions whether ##ds^2=0## holds for all metrics and spacetimes, leading to a consensus that it is indeed true across all metrics.

Areas of Agreement / Disagreement

While there is agreement that ##ds^2=0## applies to light-like curves in various metrics, there is ongoing discussion about the implications and interpretations of this condition, particularly regarding different metrics and conventions. Some aspects remain contested, particularly the implications of sign conventions for time-like world lines.

Contextual Notes

Participants mention the dependence on definitions and sign conventions for metrics, which may affect the interpretation of ##ds^2## for different types of world lines.

Arman777
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In FLWR metric or in Minkowski metric or in any general metric can we say that ##ds^2=0## cause speed of light should be constant to all observers ?

Or there's another reason ?
 
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What do you mean? What ##ds^2## is depends on the world-line you are considering. ##ds^2 = 0## corresponds to a light-like curve. This is a coordinate independent statement and it will be true for the light-like curve regardless of the coordinate system you use.
 
In FLRW metric when we measure the redshift we assume ##ds^2=0##. Like also in minkowski metric ##ds^2=0## cause only in that case we can get c=dx/dt.

Probably I should add to the question why for a light ##ds^2=0##...
 
Arman777 said:
In FLRW metric when we measure the redshift we assume ##ds^2=0##.

This is not a measurement of redshift. It is a computation of the redshift based on the FLRW universe. Studying light, it is quite clear that we must use a light-like geodesics.

Like also in minkowski metric ##ds^2=0## cause only in that case we can get c=dx/dt.

Probably I should add to the question why for a light ##ds^2=0##...

Light is massless and moves along null geodesics.
 
Orodruin said:
This is not a measurement of redshift. It is a computation of the redshift based on the FLRW universe. Studying light, it is quite clear that we must use a light-like geodesics.

Hmm I see, I ll do more research on light-like geodesic case.

I haven't seen it yet so I was confused about the reason. I guess I can understand why we use ##ds^2=0##.
 
Arman777 said:
In FLRW metric when we measure the redshift we assume ds2=0ds2=0ds^2=0.
The redshift you are talking about is for light. Light travels on null geodesics. Therefore ##ds^2=0##. It is not a general statement about the metric, it is a specific statement about light.

Arman777 said:
Like also in minkowski metric ds2=0ds2=0ds^2=0 cause only in that case we can get c=dx/dt.
Same thing here. For light ##ds^2=0## for the reason you gave. But for massive objects ##ds^2<0## and for hypothetical tachyons ##ds^2>0##.

Arman777 said:
Probably I should add to the question why for a light ds2=0ds2=0ds^2=0...
If you write down the metric, set ##ds^2=0##, then what are you left with? The equation of a sphere of radius ##ct##. This is something traveling at c in all directions, which is the second postulate. Therefore, ##ds^2=0## for light is the mathematical statement of the second postulate.
 
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Dale said:
Same thing here. For light ##ds^2=0## for the reason you gave. But for massive objects ##ds^2<0## and for hypothetical tachyons ##ds^2>0##.
I think it should be qualified that whether ##ds^2 > 0## or ##ds^2 < 0## for time-like world lines depends on the sign convention for the metric. Mathematicians and GR people generally prefer ##ds^2 < 0## while particle physicists prefer ##ds^2 > 0##. Always check which convention is being used in the particular text. Of course, this does not affect ##ds^2 = 0## for null world lines.
 
Orodruin said:
I think it should be qualified that whether ds2>0ds2>0ds^2 > 0 or ds2<0ds2<0ds^2 < 0 for time-like world lines depends on the sign convention for the metric.
Yes, good point. My preferred convention is to write ##ds^2## when I am using the (-+++) convention and to write ##d\tau^2## when I am using the (+---) convention
 
Dale said:
It is not a general statement about the metric, it is a specific statement about light.
Yes I tried to mean that, as I understood from your post for light ##ds^2=0##. But Is this true for all of the metrics ?
In example For Minkowski metric we are working on light rays then ##ds^2=0##, in FLRW metric , we are working on light then ##ds^2=0## etc. ?

Or there could be a metric where we can't set ##ds^2=0## for light ?

Dale said:
If you write down the metric, set ds2=0ds2=0ds^2=0, then what are you left with? The equation of a sphere of radius ctctct. This is something traveling at c in all directions, which is the second postulate. Therefore, ds2=0ds2=0ds^2=0 for light is the mathematical statement of the second postulate.
I see, thanks
Also,
Orodruin said:
Light is massless and moves along null geodesics.
I understand it now
 
  • #10
Arman777 said:
But Is this true for all of the metrics ?
Yes, it is true for all metrics and all spacetimes
 
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  • #11
Dale said:
Yes, it is true for all metrics and all spacetimes
Thanks a lot
 

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