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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 ?
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