The gluon density in protons and nuclei has been observed to increase very rapidly with energy. At high energies, however, nonlinear effects of QCD start to become important, slowing down the evolution of the gluon density and hence giving rise to gluon saturation. This gluon saturation can be naturally described using the Color-Glass Condensate (CGC) effective field theory. In practice, descriptions using CGC often employ the so-called infinite-target limit which neglects the dependence on the impact parameter in the collision. In this talk, I will discuss the effects of including a finite size for the target and argue that neglecting the impact parameter can lead to misleading results for proton targets.