The major stepsThe dynamics of standard cosmology has two parts: firstly, the dynamics of the background spatially homogeneous and isotropic Friedmann-Lemaître-Robertson-Walker ('FLRW') model; and secondly, the dynamics of inhomogeneous perturbations about that model that lead to structure formation in the expanding universe. Understanding each has taken place in two phases: before inflation theory, and after inflation theory. The 1946 Lifshitz paper reprinted here "On the gravitational stability of the expanding universe" [1,2] was the pioneer paper investigating the development of generic linearised inhomogeneities, and provided the basis for all further developments in this regard.Cosmological models must of course be related to astronomical observations. One can observationally directly test the geometry of the background model, and can observe the structures that form in this model. However additionally, observational studies of large scale structures on the one hand, and of Cosmic Microwave Background Radiation ('CMB') anisotropies on the other, provide strong observational constraints on the background model [3,4].The republication of the original paper can be found in this issue following the editorial note and online via doi:10.1007/s10714-016-2165-8.