A quantitative comparison between and elements for solving the CahnaHilliard equation

The CahnaHilliard (CH) equation is a time-dependent fourth-order partial differential equation (PDE). When solving the CH equation via the finite element method (FEM), the domain is discretized by C 1 -continuous basis functions or the equation is split into a pair of second-order PDEs, and discreti...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Journal of computational physics 2013-03, Vol.236, p.74-80
Hauptverfasser: Zhang, Liangzhe, Tonks, Michael R, Gaston, Derek, Peterson, John W, Andrs, David, Millett, Paul C, Biner, Bulent S
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Beschreibung
Zusammenfassung:The CahnaHilliard (CH) equation is a time-dependent fourth-order partial differential equation (PDE). When solving the CH equation via the finite element method (FEM), the domain is discretized by C 1 -continuous basis functions or the equation is split into a pair of second-order PDEs, and discretized via C 0 -continuous basis functions. In the current work, a quantitative comparison between C 1 Hermite and C 0 Lagrange elements is carried out using a continuous Galerkin FEM formulation. The different discretizations are evaluated using the method of manufactured solutions solved with Newton's method and Jacobian-Free Newton Krylov. It is found that the use of linear Lagrange elements provides the fastest computation time for a given number of elements, while the use of cubic Hermite elements provides the lowest error. The results offer a set of benchmarks to consider when choosing basis functions to solve the CH equation. In addition, an example of microstructure evolution demonstrates the different types of elements for a traditional phase-field model.
ISSN:0021-9991