Sensitive polymer gels consist of swollen networks of crosslinked macromolecules subject to a delicate interplay with their environment, allowing them to be swollen and deswollen or crosslinked and decrosslinked upon external stimulation. Such environmental sensitivity can be realized by the use of covalently crosslinked polymer networks that exhibit critical miscibility with their swelling medium or by the use of transient and reversible, supramolecular chain crosslinking. Both classes of sensitive gels are established and used in a variety of applications. However, to make this truly useful, systematic relations between the structure, dynamics, and properties of these gels must be derived. In addition to the specific trigger of gel responsiveness, a prime factor of influence in this interplay is the nanostructural polymer‐network topology. Whereas a simplistic view of a polymer network is that of an ideal, regular array of monodisperse meshes, real polymer networks often display polydisperse mesh sizes, along with structural imperfections such as loops and dangling chains, and along with further spatial inhomogeneities of their crosslinking density on a length scale of several tens of nanometers. This article summarizes recent effort to consistently probe the impact and temporal evolution of such nanostructural complexity in both gels with critical polymer–solvent miscibility and in gels with transient supramolecular crosslinking. For this purpose, different designed model systems are introduced to control and probe the polymer‐network nanostructural heterogeneity as an experimental variable. This is done using techniques such as rheology, fluorescence recovery after photobleaching, light scattering, and neutron scattering.