If you’re dealing with general relativity, there’s no way to avoid gravity. You can pick a reference frame where you’re not accelerating at the origin, but if you look at a path epsilon away then it will be accelerating against the tidal forces.
If you’re dealing with general relativity, there’s no way to avoid gravity. You can pick a reference frame where you’re not accelerating at the origin, but if you look at a path epsilon away then it will be accelerating against the tidal forces.