scholarly journals An anisotropic phase-field model for solid-state dewetting and its sharp-interface limit

Nonlinearity ◽  
2017 ◽  
Vol 30 (4) ◽  
pp. 1465-1496 ◽  
Author(s):  
Marion Dziwnik ◽  
Andreas Münch ◽  
Barbara Wagner
2015 ◽  
Vol 48 (1) ◽  
pp. 394-395 ◽  
Author(s):  
Marion Dziwnik ◽  
Andreas Münch ◽  
Barbara Wagner

2010 ◽  
Vol 140 (6) ◽  
pp. 1161-1186 ◽  
Author(s):  
Wolfgang Dreyer ◽  
Christiane Kraus

We study the thermodynamic consistency of phase-field models, which include gradient terms of the density ρ in the free-energy functional such as the van der Waals–Cahn–Hilliard model. It is well known that the entropy inequality admits gradient and higher-order gradient terms of ρ in the free energy only if either the energy flux or the entropy flux is represented by a non-classical form. We identify a non-classical entropy flux, which is not restricted to isothermal processes, so that gradient contributions are possible.We then investigate equilibrium conditions for the van der Waals–Cahn–Hilliard phase-field model in the sharp interface limit. For a single substance thermodynamics provides two jump conditions at the sharp interface, namely the continuity of the Gibbs free energies of the adjacent phases and the discontinuity of the corresponding pressures, which is balanced by the mean curvature. We show that these conditions can be also extracted from the van der Waals–Cahn–Hilliard phase-field model in the sharp interface limit. To this end we prove an asymptotic expansion of the density up to the first order. The results are based on local energy estimates and uniform convergence results for the density.


2016 ◽  
Vol 354 (10) ◽  
pp. 986-992 ◽  
Author(s):  
Leonid Berlyand ◽  
Mykhailo Potomkin ◽  
Volodymyr Rybalko

2016 ◽  
Vol 54 (3) ◽  
pp. 1558-1584 ◽  
Author(s):  
Luise Blank ◽  
Harald Garcke ◽  
Claudia Hecht ◽  
Christoph Rupprecht

2017 ◽  
Vol 12 (4) ◽  
pp. 551-590 ◽  
Author(s):  
Leonid Berlyand ◽  
◽  
Mykhailo Potomkin ◽  
Volodymyr Rybalko ◽  

2020 ◽  
Vol 229 (19-20) ◽  
pp. 2899-2909
Author(s):  
L. V. Toropova ◽  
P. K. Galenko ◽  
D. V. Alexandrov ◽  
M. Rettenmayr ◽  
A. Kao ◽  
...  

Author(s):  
T. Philippe ◽  
H. Henry ◽  
M. Plapp

At equilibrium, the shape of a strongly anisotropic crystal exhibits corners when for some orientations the surface stiffness is negative. In the sharp-interface problem, the surface free energy is traditionally augmented with a curvature-dependent term in order to round the corners and regularize the dynamic equations that describe the motion of such interfaces. In this paper, we adopt a diffuse interface description and present a phase-field model for strongly anisotropic crystals that is regularized using an approximation of the Willmore energy. The Allen–Cahn equation is employed to model kinetically controlled crystal growth. Using the method of matched asymptotic expansions, it is shown that the model converges to the sharp-interface theory proposed by Herring. Then, the stress tensor is used to derive the force acting on the diffuse interface and to examine the properties of a corner at equilibrium. Finally, the coarsening dynamics of the faceting instability during growth is investigated. Phase-field simulations reveal the existence of a parabolic regime, with the mean facet length evolving in t , with t the time, as predicted by the sharp-interface theory. A specific coarsening mechanism is observed: a hill disappears as the two neighbouring valleys merge.


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