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Numerical studies of the fingering phenomena for the thin film equation
Author(s) -
Li Yibao,
Lee Hyun Geun,
Yoon Daeki,
Hwang Woonjae,
Shin Suyeon,
Ha Youngsoo,
Kim Junseok
Publication year - 2010
Publication title -
international journal for numerical methods in fluids
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.938
H-Index - 112
eISSN - 1097-0363
pISSN - 0271-2091
DOI - 10.1002/fld.2420
Subject(s) - nonlinear system , mechanics , front (military) , viscous fingering , multigrid method , context (archaeology) , partial differential equation , regular polygon , mathematical analysis , mathematics , euler equations , materials science , physics , geometry , porous medium , composite material , geology , paleontology , quantum mechanics , porosity , meteorology
We present a new interpretation of the fingering phenomena of the thin liquid film layer through numerical investigations. The governing partial differential equation is h t + ( h 2 − h 3 ) x = −∇·( h 3 ∇Δ h ), which arises in the context of thin liquid films driven by a thermal gradient with a counteracting gravitational force, where h = h ( x, y, t ) is the liquid film height. A robust and accurate finite difference method is developed for the thin liquid film equation. For the advection part ( h 2 − h 3 ) x , we use an implicit essentially non‐oscillatory (ENO)‐type scheme and get a good stability property. For the diffusion part −∇·( h 3 ∇Δ h ), we use an implicit Euler's method. The resulting nonlinear discrete system is solved by an efficient nonlinear multigrid method. Numerical experiments indicate that higher the film thickness, the faster the film front evolves. The concave front has higher film thickness than the convex front. Therefore, the concave front has higher speed than the convex front and this leads to the fingering phenomena. Copyright © 2010 John Wiley & Sons, Ltd.