In the EOS pV=f (T) one needs two parameters to determine the third. In this case, knowing the final pressure, temperature would be necessary and sufficient.
If the compression path is fully identified one could estimate the other macroscopic properties, given the final pressure, for example:
P1V1=P2V2 refers to an isothermic process, while
P1V1[γ] = constant, to an adiabatic process.
BTW, compression can follow a variety of paths, e.g., isothermic, adiabatic, even isochoric. We can compress a gas at constant volume (!) by the addition of heat.