Abstract. Dewetting instabilities cause a thin liquid film coating a solid substrate to rupture and finally form complex patterns, which are quasiequilibrium parabolic droplets connected by an ultra thin residual film. During the Ostwald ripening process, droplets exchange mass through the residual thin film without touching each other. Bigger ones grow while smaller ones shrink and disappear. As a result the total number of droplets N (t) decreases while the average size increases. For the physically realistic case when the underlying substrate is two dimensional, it is predicted that the average volume of droplets V follows a temporal power-logarithmic law: V 4/3 lnV ∼ ct. We propose a mean field model for the Ostwald ripening of 2D thin films and define a structural time scale ts, which is heuristically similar to t. In this mean field model we rigorously prove that V can not grow faster than the power-logarithmic law in ts in the average sense, as long as the droplets are well separated.Key words. Thin film equation, coarsening, Ostwald ripening, mean field models.AMS subject classifications. 35B40, 76A20, 35K25, 35K55, 35Q80.
IntroductionDue to the dewetting instabilities, a thin liquid film coating a solid substrate goes through complicated morphological changes and ultimately forms complex nonlinear patterns in the late stage. The patterns are essentially quasi-static fluid droplets connected by an ultra thin residual film. Droplets may exchange mass through a diffusion field in the ultra thin film. Smaller ones shrink and collapse while bigger ones grow. This mechanism is called Ostwald ripening, as it is similar to what happens in phase transitions (see, e.g., [22]). Meanwhile, droplets may move around and collide to form bigger ones. These two mechanisms cause coarsening phenomena to occur where we observe the decrease of the total number of droplets and an increase in the average droplet size and the average distance between droplets.For the simplified case when the underlying substrate is one-dimensional, the coarsening dynamics of the thin film was studied by Glasner and Witelski [10,12] using asymptotic analysis methods. Heuristic arguments and numerical simulations suggest that under both mechanisms the number of droplets N (t) decreases following a temporal power law N (t) ∼ ct −2/5 . As a consequence, the average distance between drops grows as a temporal power law t 2/5 and the average height and width of drops grow as t 1/5 . The size distribution of droplets was studied in [13] by considering a mean field model when the ripening mechanism dominates. Their numerical simulations indicate that the power law for N (t) holds in the average sense when self-similarity of the size distribution is not attained. In [2], we studied the mean field model in [13] and rigorously proved that in the average sense N (t) can not decrease faster than the t −2/5 power law. When the underlying substrate is two dimensional, which is the physically realistic case, the situation becomes much more complicated. It is s...