The Cahn-Hilliard Equation with Logarithmic Potentials
By Laurence Cherfils, Alain Miranville, Sergey Zelik. 2011
233 citations recorded by the source corpus.
Subfields: Atmospheric Science, Computational Theory and Mathematics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/1b1beb833aaab7f33b4b6b4acb578db4e3f1f910
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In Atmospheric Science
In Computational Theory and Mathematics
In Materials Chemistry
Citations in the corpus
- Fractional Cahn-Hilliard, Allen-Cahn and porous medium equations (2015, unknown): “, [13, 28] for a comprehensive bibliography).”
- Optimal Control for the Convective Cahn–Hilliard Equation in 2D Case (2014, methodology): “[18] investigated the Cahn–Hilliard equation in phase separation with the thermodynamically relevant logarithmic potentials; Gilardi et al.”
- On a generalized Cahn-Hilliard equation with biological applications (2014, unknown): “, [2], [3], [5], [9], [16], [17], [18], [19], [23] and [24] for more details.”
- A Review on the Cahn-Hilliard Equation: Classical Results and Recent Advances in Dynamic Boundary Conditions (2021, background): “A lot of attentions have been paid to the problem (1.1)–(1.4) with a constant mobility M > 0 and a singular potential F including the typical ones (2.2) and (2.4), see [27,41,58] for some surveys on this topic.”
- On the maximum principle preserving schemes for the generalized Allen–Cahn equation (2016, background): “More details about the latter one can be found in [3, 4].”
- The nonlocal Cahn–Hilliard equation with singular potential: Well-posedness, regularity and strict separation property (2017, background): “1) with constant mobility can be found in [16].”
- Longtime behavior of nonlocal Cahn-Hilliard equations (2012, background): “iard equation was proposed in [7] as a model for (isothermal) phase separation phenomena in binary alloys. Since then it was analyzed by many authors and used in several different contexts (see, e.g., [9, 40] and references therein). The basic form of such an equation is the following (1.1) ∂tϕ= ∇ ·[”