In the thesis we consider the classic problem of a compact matter source (a perfect
fluid) that evolves under the assumption of slow motion and weak gravitational
field. The non-relativistic evolution of the system leads to a separation of scales.
This allows us to solve for the metric near the source (the near zone) using a
post-Newtonian expansion while outside (the exterior zone) the source we apply
a multipolar post-Minkowskian expansion. Due to the separation of scales the
exterior zone and the near zone will overlap which allows us to glue the two
expansions together using matched asymptotic expansion methods. Standard
approaches like that of Blanchet-Damour or the DIRE approach rely entirely on
harmonic gauge. In this thesis we set up the framework to allow for any gauge
with a Newtonian regime which we will refer to as post-Newtonian gauges. With
this we are able to make broad statements about the structure of the expansion
and the equations of motion in any post-Newtonian gauge and to arbitrary orders
in both the near zone and the exterior zone expansions. We check that our
framework correctly reproduces the near zone metric in harmonic gauge to 2.5
post-Newtonian order. Finally, we apply our framework to the transverse gauge
which can be thought of as the general relativity equivalent of the Coulomb gauge
in electromagnetism. We explicitly compute the near zone metric in transverse
gauge to 2.5 post-Newtonian order as well as the far zone metric up to 1 post-Newtonian order beyond the quadrupole formula
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