Derivation of Lorentz law in Curved Spacetime?
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Hey mate!
In the presence of external forces or rather presence of fields to which a particle "couples" in curved spacetime.
Ex:
S[γ;A]=∫dλmgγ(λ)(vγ,γ(λ),vγ,γ(λ)−√+qA(vγ,γ(λ))
where mm is the mass of the particle and A is a co-vector field (electromagnetic potential) on the Manifold.
Thanks for the question!
☺☺
In the presence of external forces or rather presence of fields to which a particle "couples" in curved spacetime.
Ex:
S[γ;A]=∫dλmgγ(λ)(vγ,γ(λ),vγ,γ(λ)−√+qA(vγ,γ(λ))
where mm is the mass of the particle and A is a co-vector field (electromagnetic potential) on the Manifold.
Thanks for the question!
☺☺
Answered by
0
In special relativity (flat spacetime), if Christoffel symbols are not allowed in writing the laws of physics, then Lorentz transformations will preserve
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