{ "id": "2408.06836", "version": "v1", "published": "2024-08-13T11:50:02.000Z", "updated": "2024-08-13T11:50:02.000Z", "title": "Linear stability analysis of a vertical liquid film over a moving substrate", "authors": [ "Fabio Pino", "Miguel Alfonso Mendez", "Benoit Scheid" ], "categories": [ "physics.flu-dyn", "math-ph", "math.MP" ], "abstract": "The stability of liquid film flows are important in many industrial applications. In the dip-coating process, a liquid film is formed over a substrate extracted at a constant speed from a liquid bath. We studied the linear stability of this film considering different thicknesses $\\hat{h}$ for four liquids, spanning a large range of Kapitza numbers ($\\rm Ka$). By solving the Orr-Sommerfeld eigenvalue problem with the Chebyshev-Tau spectral method, we calculated the neutral curves, investigated the instability mechanism and computed the absolute/convective threshold. The instability mechanism was studied through the analysis of vorticity distribution and the kinetic energy balance of the perturbations. It was found that liquids with low $\\rm Ka$ (e.g. corn oil, $\\text{Ka}$ = 4) have a smaller area of stability than a liquid at high $\\rm Ka$ (e.g. Liquid Zinc, $\\rm Ka$ = 11525). Surface tension has both a stabilizing and a destabilizing effect, especially for large $\\rm Ka$. For long waves, it curves the vorticity lines near the substrate, reducing the flow under the crests. For short waves, it fosters vorticity production at the interface and creates a region of intense vorticity near the substrate. In addition, we discovered that the surface tension contributes to both the production and dissipation of perturbation's energy depending on the $\\rm Ka$ number. In terms of absolute/convective threshold, we found a window of absolute instability in the $\\text{Re}-\\hat{h}$ space, showing that the Landau-Levich-Derjaguin solution ($\\hat{h}=0.945 \\text{Re}^{1/9}\\text{Ka}^{-1/6}$) is always convectively unstable. Moreover, we show that for $\\text{Ka}<17$, the Derjaguin's solution ($\\hat{h}=1$) is always convectively unstable.", "revisions": [ { "version": "v1", "updated": "2024-08-13T11:50:02.000Z" } ], "analyses": { "keywords": [ "linear stability analysis", "vertical liquid film", "moving substrate", "instability mechanism", "fosters vorticity production" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }