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Lattice Boltzmann modeling of contact angle and its hysteresis in two-phase flow with large viscosity difference

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Figure

FIG. 2: Contact angle as a function of Θw for the viscosity ratios M = 1 (represented by triangles) and 100 (represented bycircles)
FIG. 3: Simulation setup for capillary intrusion. The portion in the center of the domain is a capillary tube of length Lwidth and r
FIG. 5: Schematic diagram of a droplet meniscus on a non-ideal substrate subject to a simple shear flow.
FIG. 6: Comparison of the simulated equilibrium droplet shapes with the numerical results of Schleizer and Bonnecaze [74]for Ca = 0.05, 0.1, and 0.15 at A∗d = 0.5
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