Well-posedness and stability of the self-similar profile for a thin-film equation with gravity
Manuel V. Gnann, Slim Ibrahim
TL;DR
This work proves well-posedness and stability for perturbations of a non-explicit self-similar profile of a thin-film equation with gravity. It uses a mass-Lagrangian reformulation and a weighted $L^2$ gradient-flow framework around the self-similar state, establishing a coercive Hessian and maximal-regularity estimates for the linearized problem, then controlling the nonlinear terms to obtain global existence and decay. The main results show convergence toward the self-similar profile in weighted Sobolev norms, with explicit asymptotics in the original variables: the height decays like $t^{-1/5}$ and the contact-line velocity decays like $t^{-4/5}$, up to perturbative corrections. Importantly, the approach avoids requiring an explicit algebraic representation of the self-similar profile, offering a flexible toolbox for analyzing stability of special solutions in related degenerate-diffusion problems.
Abstract
We consider the thin-film equation with linear mobility and a stabilizing second-order porous-medium type term modeling gravity. The model admits self-similar solutions, and our goal is to analyze their stability. We reformulate the problem in mass-Lagrangian coordinates and exploit the underlying gradient-flow structure of the equation with respect to a weighted $L^2$ inner product, where the weight is given by the self-similar source-type profile. This framework allows us to establish a coercivity result for the Hessian (the linearization around the self-similar solution) in a suitably weighted inner product. As a consequence, we prove the convergence of perturbations toward the self-similar profile at an algebraic rate of order $t^{-\frac 1 5}$, in arbitrary scales of weighted Sobolev norms. The analysis relies on maximal-regularity estimates for the linearized evolution, combined with appropriate estimates for the nonlinear terms. Notably, beyond perturbative regimes and in contrast to previous results for the thin-film equation (convergence to the Smyth-Hill profile) or the porous-medium equation (convergence to the Barenblatt-Pattle solution), our analysis does not rely on an explicit (algebraic) representation of the self-similar profile. Instead, it is based solely on a systematic use of the ordinary differential equation satisfied by the self-similar solution, together with a careful analysis of its boundary asymptotics. As a result, we expect that the approach developed here can serve as a flexible toolbox for the study of more general classes of equations and for the stability analysis of special solutions in future work.
