2016
DOI: 10.1002/num.22121
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Error estimates of fully discrete finite element solutions for the 2D Cahn–Hilliard equation with infinite time horizon

Abstract: In this article, we deal with a rigorous error analysis for the finite element solutions of the two‐dimensional Cahn–Hilliard equation with infinite time. The L 2 − H 1 error estimates with respect to ( h , τ ) are proven for the fully discrete conforming piecewise linear element solution under Assumption (A1) on the initial value and Assumption (A2) on the discrete spectrum estimate in the finite element space. The analysis is based on sharp a‐priori estimates for the solutions, particularly ref… Show more

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Cited by 9 publications
(4 citation statements)
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“…Variable ϕ is a phase function, assumes distinct values ±1 to indicate two materials, and continuously varies through the thin interface transition layer with thickness proportional to the parameter ϵ [ 14 ] . Equation (1) shows the tendencies of mixing and separation according to the first term and second term, which result in the equilibrium pattern for the interface due to competition between two types of interactions [25, 47]. We take the double well free energy Ffalse(ϕfalse)=14(ϕ21)2 thereafter in this paper.…”
Section: Cahn–hilliard–darcy Systemmentioning
confidence: 99%
See 1 more Smart Citation
“…Variable ϕ is a phase function, assumes distinct values ±1 to indicate two materials, and continuously varies through the thin interface transition layer with thickness proportional to the parameter ϵ [ 14 ] . Equation (1) shows the tendencies of mixing and separation according to the first term and second term, which result in the equilibrium pattern for the interface due to competition between two types of interactions [25, 47]. We take the double well free energy Ffalse(ϕfalse)=14(ϕ21)2 thereafter in this paper.…”
Section: Cahn–hilliard–darcy Systemmentioning
confidence: 99%
“…Theorem 1 Let (u, p, 𝜙, 𝜇) be smooth solution of the variational form ( 21)- (25) with the initial condition (7). Then solution (u, p, 𝜙, 𝜇) satisfies the mass conservation, that is,…”
Section: Weak Formulationmentioning
confidence: 99%
“…b(u) is the non-negative diffusion mobility and Ψ(u) is the homogeneous free energy density. Based on the development of the model in Cahn-Hilliard equation, it is not surprising that many different numerical methods have been proposed for the Cahn-Hilliard equation, including the finite element methods [4][5][6][7][8][9][10][11][12][13], discontinuous Galerkin methods [14][15][16], local discontinous Galerkin methods [3,17,18], multi-grid method [19][20][21], finite difference methods [22][23][24] and so on. Second, the Camassa-Holm equations, introduced by Camassa and Holm in [25,26] as a model for the shallow water motion on the flat surface, are one of the basic models of peaked solitons.…”
Section: Introductionmentioning
confidence: 99%
“…Liu and Shen in 2015 constructed a stabilized semi-implicit spectral deferred correction methods in time discretization for Allen-Cahn and Cahn-Hilliard equations with the Legendre-Galerkin approximation in space [20]. There are many other significant works that deal with the Allen-Cahn and Cahn-Hiliiard equations [34,15,28,16,30,32,24,21,12,18,14,22,27].…”
mentioning
confidence: 99%