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| sci.physics.relativity | The theory of relativity | 225,861 messages |
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| Message 225,056 of 225,861 |
| Paul B. Andersen to All |
| Re: Gravitational redshift/blueshift |
| 04 Dec 25 10:48:54 |
From: relativity@paulba.no Den 03.12.2025 23:25, skrev Paul B. Andersen: > > ds² = - c²dτ² = -(1 − 2GM/[c²r])c²dt² + 1/(1 − 2GM/[c²r])dr² > + r² (dθ² + sin² θ dφ) > Which is correct. > > When s² < 0 and thus time like, then (-c²τ²) < 0 and thus time like. > > So : ds² = -(1 − 2GM/[c²r])c²dt² + 1/(1 − 2GM/[c²r])dr² > + r² (dθ² + sin² θ dφ) > and: -c²dτ² = -(1 − 2GM/[c²r])c²dt² + 1/(1 − 2GM/[c²r])dr² > + r² (dθ² + sin² θ dφ) .. are the same metric. -- Paul https://paulba.no/ --- SoupGate-Win32 v1.05 * Origin: you cannot sedate... all the things you hate (1:229/2) |
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