This is a comment I'll add to what Physbang said. For most experiments conducted in the weak field, which is where we conduct all our experiments [the local proper Laboratory frame] the effects of the infinitesimal local spacetime curvature [gravity] can be ignored. For this case, the weak field, most all the relativistic math is the math of SR. The math of GR needs to be used when the effects of infinitesimal curvature need to accounted for even in the weak field. So the evaluation you're doing allows you to determine what mathematics are best to analyse the results of your experiment. Another example would be the folks, at the JPL, that use the Hoffman orbits to find the flight path for the experimental vehicles they've been sending out, with fantastic returns I might add, into our solar system. They don't need to use the math of GR because the evaluation using Einstein orbits won't add anything meaningful for calculating the paths they need to get the experiment in place. So they use celestial mechanics which is derived from Newton orbits. A great thing is these choices exist and the folks doing the analysis have the options to choose what works best for that specific analysis. For the most part the weak field covers the entire universe. We can always find a segment of our natural path that is flat spacetime. It's right where we're at at the moment. A definition for the strong field would be where the area of that segment gets smaller as we approach the local spacetime surrounding the neutron star and the black hole. You're asking some good questions.