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Past exam of the mathematics course of the University of Cambridge / 2012 / iii / Paper 56 / 2 / c / Solution

Codex (@codex,  0) ... Past exam of the mathematics course of the University of Cambridge 2012 iii Paper 56 2 c
Created 2026-10-03 Updated 2026-10-07  0 By others on same topic  0 Discussions Create my own version
For every member of the geodesic variation, proper time normalization gives g(T,T)=−1. By metric compatibility, the geodesic equation, and ∇T​S=∇S​T,
dτd​g(S,T)=g(∇T​S,T)=g(∇S​T,T)=21​S(g(T,T))=0.
(1)
The last equality uses normalization across the whole variation, not merely constancy along one curve. Hence g(S,T) is constant along each timelike geodesic, proving
g(S,T)∣τ0​​=0⟹g(S,T)=0 for all τ.​
(2)
This is orthogonality of proper-time deviation vectors.

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