Faraday instability of binary miscible/immiscible fluids with phase field approach

2021 ◽  
Vol 6 (6) ◽  
Author(s):  
M. Bestehorn ◽  
D. Sharma ◽  
R. Borcia ◽  
S. Amiroudine
2010 ◽  
Vol 643 ◽  
pp. 127-136 ◽  
Author(s):  
GUIDO BOFFETTA ◽  
ANDREA MAZZINO ◽  
STEFANO MUSACCHIO ◽  
LARA VOZELLA

The effects of polymer additives on Rayleigh–Taylor (RT) instability of immiscible fluids is investigated using the Oldroyd-B viscoelastic model. Analytic results obtained exploiting the phase-field approach show that in polymer solution the growth rate of the instability speeds up with elasticity (but remains slower than in the pure solvent case). Numerical simulations of the viscoelastic binary fluid model confirm this picture.


Author(s):  
Sindhu Nagaraja ◽  
Kay Leichsenring ◽  
Marreddy Ambati ◽  
Laura De Lorenzis ◽  
Markus Böl

2020 ◽  
Author(s):  
D. Kay ◽  
V. Styles ◽  
A. Münch ◽  
Q. Parsons

Author(s):  
Christian Rohde ◽  
Lars von Wolff

We consider the incompressible flow of two immiscible fluids in the presence of a solid phase that undergoes changes in time due to precipitation and dissolution effects. Based on a seminal sharp interface model a phase-field approach is suggested that couples the Navier–Stokes equations and the solid’s ion concentration transport equation with the Cahn–Hilliard evolution for the phase fields. The model is shown to preserve the fundamental conservation constraints and to obey the second law of thermodynamics for a novel free energy formulation. An extended analysis for vanishing interfacial width reveals that in this limit the sharp interface model is recovered, including all relevant transmission conditions. Notably, the new phase-field model is able to realize Navier-slip conditions for solid–fluid interfaces in the limit.


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