Answers to Where do gravitational field lines go exactly? We know where they start, but explain that for Newtonian gravity they go to infinity.
In a simple Newtonian gravity exercise there is no "speed of gravity" consideration. At any moment we can calculate the potential field from integrating $-G \rho(r) / r$ where $r$ is the distance to each element. The force field comes from the gradient of that potential and we can draw gravitational field lines in order to look at them by starting at some point and integrating the normal of the force.
There is this comment which informs us
We don't use field lines for gravity outside of Newtonian gravity. But (this) answer is also correct.
I was hoping that that comment would have evolved into a second answer which would have provided enough space in which to expand on it. Instead I'll ask here:
Question: Are gravitational field lines ever used in situations beyond classical Newtonian gravity? If so, must they still "go to infinity" or might they do more interesting things?