HomogenousCow
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If you simply interpret the RHS of the geodesic equation as a four-acceleration, can't we just treat gravity as a force?
The discussion revolves around the interpretation of gravity within the framework of general relativity, particularly whether gravity can be treated as a force. Participants explore the implications of the geodesic equation, fictitious forces, and the nature of gravitational effects in different coordinate systems.
Participants express differing views on whether gravity can be treated as a force, with some supporting the idea and others contesting it. The discussion remains unresolved, with multiple competing interpretations of gravity's nature and its relationship to fictitious forces.
There are limitations in the discussion regarding the assumptions made about the geodesic equation and the definitions of fictitious forces. The implications of these interpretations are not fully resolved, and the mathematical steps involved in the arguments are not detailed.
Murphrid is correct. You can certainly move the term involving Christoffel symbols to the other side from the term involving the coordinate acceleration, but the resulting equation is no longer a tensor equation and does not transform as a tensor does.HomogenousCow said:If you simply interpret the RHS of the geodesic equation as a four-acceleration, can't we just treat gravity as a force?