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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 ?
Or there's another reason ?
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.
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.
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 said: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##...
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.
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:In FLRW metric when we measure the redshift we assume ds2=0ds2=0ds^2=0.
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:Like also in minkowski metric ds2=0ds2=0ds^2=0 cause only in that case we can get c=dx/dt.
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.Arman777 said:Probably I should add to the question why for a light ds2=0ds2=0ds^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.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##.
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 (+---) conventionOrodruin 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 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 ?Dale said:It is not a general statement about the metric, it is a specific statement about light.
I see, thanksDale 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 understand it nowOrodruin said:Light is massless and moves along null geodesics.
Yes, it is true for all metrics and all spacetimesArman777 said:But Is this true for all of the metrics ?
Thanks a lotDale said:Yes, it is true for all metrics and all spacetimes