We investigate spherically symmetric spacetimes with an anisotropic fluid and discuss the existence and stability of a dividing shell separating expanding and collapsing regions. We find that the dividing shell is defined by a relation between the pressure gradients, both isotropic and anisotropic, and the strength of the fields induced by the Misner-Sharpe mass inside the separating shell and by the pressure fluxes. This balance is a generalization of the Tolman-OppenheimerVolkoff equilibrium condition which defines a local equilibrium condition, but conveys also a nonlocal character given the definition of the Misner-Sharpe mass. We present a particular solution with dust and radiation that provides an illustration of our results.The universe close to us exhibits structures below certain scales that seem to be immune to the overall expansion of the universe. This reflects two different gravitational behaviors, and usually the dynamics corresponding to the structures that have undergone non-linear collapse is treated under the approximation that Newton's gravitational theory is valid without residual acceleration. However, this approach does not tell us with exactitude what is the critical scale where the latter approximation starts to be valid, nor does it explain in a non-perturbative way how the collapse of over-dense patches decouples from the large-scale expansion. For this purpose one requires a fully general relativistic approach where an exact solution exhibiting the two competing behaviors and allowing us to characterize how the separation between them comes about. It is the understanding of this interplay between collapsing and expanding regions within the theory of general relativity (GR) that we aim to address here.In previous works we have investigated the present issue in models with spherical symmetry and with a perfect fluid [1, 2] . Here we briefly report our findings when we overcome the limitations of a perfect fluid description of the non-equilibrium setting under focus. We thus consider here an anisotropic fluid.We resort to a 3 + 1 splitting, and assess the existence and stability of a dividing shell separating expanding and collapsing regions, in a gauge invariant way.