Abstract:In this work, we propose a numerical method based on high degree continuous nodal elements for the Cahn-Hilliard evolution. The use of the p-version of the finite element method proves to be very efficient avoiding difficult computations or strategies like C 1 elements, adaptive mesh refinement, multi-grid resolution or isogeometric analysis. Beyond the classical benchmarks and comparisons with other existing methods, a numerical study has been carried out to investigate the influence of a polynomial approxima… Show more
“…We take the inner product in H(ω * h ) of this equation and µ and owing to formula (19) and the second boundary condition (33) get…”
Section: 2mentioning
confidence: 99%
“…Other polynomial approximations can be obtained by applying the Taylor expansion of Ψ sep (C) [14,19].…”
mentioning
confidence: 99%
“…Now we take the inner product in H(ω hk,l * ,m * ) of the momentum balance equation (21) and u k , replace k with i and sum up the results in i = 1, 2, 3. Using the formula 2 , the first formula (19) two times together with the first boundary condition (31) and (32) as well as formula (18) together with (32) we obtain…”
mentioning
confidence: 99%
“…We take the inner product in H(ω * h ) of the equation and µ, see (29), apply both formulas (19) together with the boundary conditions (33) and get…”
We consider the initial-boundary value problem for the 3D regularized compressible isothermal Navier-Stokes-Cahn-Hilliard equations describing flows of a two-component two-phase mixture taking into account capillary effects. We construct a new numerical semi-discrete finite-difference method using staggered meshes for the main unknown functions. The method allows one to improve qualitatively the computational flow dynamics by eliminating the so-called parasitic currents and keeping the component concentration inside the physically reasonable range (0, 1). This is achieved, first, by discretizing the non-divergent potential form of terms responsible for the capillary effects and establishing the dissipativity of the discrete full energy. Second, a logarithmic (or the Flory-Huggins potential) form for the non-convex bulk free energy is used. The regularization of equations is accomplished to increase essentially the time step of the explicit discretization in time. We include 3D numerical results for two typical problems that confirm the theoretical predictions.
“…We take the inner product in H(ω * h ) of this equation and µ and owing to formula (19) and the second boundary condition (33) get…”
Section: 2mentioning
confidence: 99%
“…Other polynomial approximations can be obtained by applying the Taylor expansion of Ψ sep (C) [14,19].…”
mentioning
confidence: 99%
“…Now we take the inner product in H(ω hk,l * ,m * ) of the momentum balance equation (21) and u k , replace k with i and sum up the results in i = 1, 2, 3. Using the formula 2 , the first formula (19) two times together with the first boundary condition (31) and (32) as well as formula (18) together with (32) we obtain…”
mentioning
confidence: 99%
“…We take the inner product in H(ω * h ) of the equation and µ, see (29), apply both formulas (19) together with the boundary conditions (33) and get…”
We consider the initial-boundary value problem for the 3D regularized compressible isothermal Navier-Stokes-Cahn-Hilliard equations describing flows of a two-component two-phase mixture taking into account capillary effects. We construct a new numerical semi-discrete finite-difference method using staggered meshes for the main unknown functions. The method allows one to improve qualitatively the computational flow dynamics by eliminating the so-called parasitic currents and keeping the component concentration inside the physically reasonable range (0, 1). This is achieved, first, by discretizing the non-divergent potential form of terms responsible for the capillary effects and establishing the dissipativity of the discrete full energy. Second, a logarithmic (or the Flory-Huggins potential) form for the non-convex bulk free energy is used. The regularization of equations is accomplished to increase essentially the time step of the explicit discretization in time. We include 3D numerical results for two typical problems that confirm the theoretical predictions.
Our aim in this article is to discuss recent issues related with the Cahn- Hilliard equation in phase separation with the thermodynamically relevant logarithmic potentials; in particular, we are interested in the well-posedness and the study of the asymptotic behavior of the solutions (and, more precisely, the existence of finite-dimensional attractors). We first consider the usual Neumann boundary conditions and then dynamic boundary conditions which account for the interactions with the walls in confined systems and have recently been proposed by physicists. We also present, in the case of dynamic boundary conditions, some numerical results
In this paper, we address the question of the discretization of Stochastic Partial Differential Equations (SPDE's) for excitable media. Working with SPDE's driven by colored noise, we consider a numerical scheme based on finite differences in time (EulerMaruyama) and finite elements in space. Motivated by biological considerations, we study numerically the emergence of reentrant patterns in excitable systems such as the Barkley or Mitchell-Schaeffer models.
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