2016
DOI: 10.1016/j.cma.2016.03.018
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A fractional phase-field model for two-phase flows with tunable sharpness: Algorithms and simulations

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Cited by 96 publications
(46 citation statements)
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“…Several numerical techniques have been recently developed for space and time non-local versions of equation (1.3), most of them based on finite differences or spectral methods [28,21,35,22,27,7]. Also, numerical methods have been studied for nonlocal versions of related phase separation models, like the Cahn-Hilliard equation [5,6].…”
Section: Introductionmentioning
confidence: 99%
“…Several numerical techniques have been recently developed for space and time non-local versions of equation (1.3), most of them based on finite differences or spectral methods [28,21,35,22,27,7]. Also, numerical methods have been studied for nonlocal versions of related phase separation models, like the Cahn-Hilliard equation [5,6].…”
Section: Introductionmentioning
confidence: 99%
“…Such an energy dissipation low plays an important role in developing stable numerical methods for dissipation systems due to its importance to the long time numerical simulation, see e.g., [12,13,14,44,36,49,16,46,42] and references therein. In recent years, fractional-type phase-field models have attracted more and more attentions [1,2,3,7,30,38,23]. For instance, consider a fractional type free energy [38] E α (φ) := Ω ε 2 2 |∇ α φ| 2 + F (φ) dx, (1.5) where ∇ α is the fractional gradient ∇ α = ( ∂ α ∂x1 , ..., ∂ α ∂x d ) and { ∂ α ∂x k } k are fractional derivatives.…”
mentioning
confidence: 99%
“…In recent years, fractional-type phase-field models have attracted more and more attentions [1,2,3,7,30,38,23]. For instance, consider a fractional type free energy [38] E α (φ) := Ω ε 2 2 |∇ α φ| 2 + F (φ) dx, (1.5) where ∇ α is the fractional gradient ∇ α = ( ∂ α ∂x1 , ..., ∂ α ∂x d ) and { ∂ α ∂x k } k are fractional derivatives. One is interested in the following space-fractional CH equation…”
mentioning
confidence: 99%
“…For spatially nonlocal phase field models, due to the spread of nonlocal interactions, the phase field variables may no longer be as smooth as their local counterpart. They may also lead to narrower interfacial region and permit singularities across the interface or at the defects [159,239,394]. 7.5.2.…”
Section: Fluid and Solid Mechanicsmentioning
confidence: 99%