The description Einstein gave us about gravity, describes gravity from the perspective of the particle, where it "feels" movement. Instead from that perspective the particle can say space-time it's self is curved and is just following a geodesic trajectory. However, if you want to take space time to be flat, because there is no gravitational force affecting you, is it possible to represent Einstein's field equations as a vector field? Possibly using the geodesic equation?
Even fictitious forces can be described as forces and both the stationary frame and the accelerated frame give the same result of where the ball ends up relative to them? This fictitious force field would need to be approximately equal to Newton's gravitational law at slow speeds, but needs to be relativistic in general. This would need to be described as a four force.
If this field can be constructed from the geodesic equation, what would the acceleration field look like as a four-vector?
If we assume a Schwarzschild metric: $$ds^2 = - (1-\frac{r_s}{r})c^2 dt^2 + \frac{1}{1-\frac{r_s}{r}} + r^2 d\Omega^2, $$
And substitute the metric into the geodesic equation: $$ {d^2 x^\mu \over d\tau^2} =- \Gamma^\mu {}_{\alpha \beta}{d x^\alpha \over d\tau}{d x^\beta \over d\tau}, $$
Is it possible to get into the form:
$$ {d^2 x^\mu \over d\tau^2} = F(x^\mu)~? $$