JOURNAL OF SHANDONG UNIVERSITY(NATURAL SCIENCE) ›› 2021, Vol. 56 ›› Issue (12): 17-25.doi: 10.6040/j.issn.1671-9352.0.2021.327

Previous Articles    

Finite element method of Cahn-Hilliard equation based on adaptive moving mesh method

LU Chang-na, CHANG Sheng-xiang   

  1. College of Mathematics and Statistics, Nanjing University of Information Science and Technology, Nanjing 210044, Jiangsu, China
  • Published:2021-11-25

Abstract: A finite element method is proposed for the two-dimensional Cahn-Hilliard equation based on the adaptive moving mesh. Since the Cahn-Hilliard equation changes rapidly in the initial stage and slowly changes in the later stage, the use of the moving mesh rule based on the moving mesh partial differential equation(MMPDE)can better capture the phase diagram. The method is discretized by using linear finite element in space and fifth-order Radau IIA scheme in time. Numerical results shows that the numerical solution can well maintain the law of conservation of mass and the law of energy stability, and improve the calculation efficiency, which verifies the effectiveness and feasibility of the method.

Key words: linear finite element, adaptive moving mesh, Cahn-Hilliard equation, energy stability

CLC Number: 

  • O242.21
[1] CAHN J W, HILLIARD J E. Free energy of a nonuniform system(I. Interfacial free energy)[J]. J Chem Phys, 1958, 28(2):258-267.
[2] LIU Chun, SHEN Jie. A phase field model for the mixture of two incompressible fluids and its approximation by a Fourier-spectral method[J]. Physica D, 2003, 179(3/4):211-228.
[3] SUN Zhizhong. A second-order accurate linearized difference scheme for the two-dimensional Cahn-Hilliard equation[J/OL]. Math Comput, 1995[2021-09-23]. https://doi.org/10.1090/S0025-5718-1995-1308465-4.
[4] FENG X B, PROHL A. Analysis of a fully discrete finite element method for the phase field model and approximation of its sharp interface limits[J/OL]. Math Comput, 2004[2021-09-23]. https://doi.org/10.1090/S0025-5718-03-01588-6.
[5] FENG Xinlong, TANG Tao, YANG Jiang. Stabilized Crank-Nicolson/Adams-Bashforth schemes for phase field models[J]. E Asian J Appl Math, 2013, 3(1):59-80.
[6] CHEN Longqing, SHEN Jie. Applications of semi-implicit Fourier-spectral method to phase field equations[J]. Comput Phys Commun, 1998, 108(2):147-158.
[7] DU Qiang, JU Lili, LI Xiao, et al. Stabilized linear semi-implicit schemes for the nonlocal Cahn-Hilliard equation[J/OL]. J Comput Phys, 2018[2021-09-23]. https://doi.org/10.1016/j.jcp.2018.02.023.
[8] LI Dong, QIAO Zhonghua, TANG Tao. Characterizing the stabilization size for semi-implicit Fourier-spectral method to phase field equations[J]. SIAM J Numer Anal, 2016, 54(3):1653-1681.
[9] XIA Yinhua, XU Yan, SHU Chiwang. Local discontinuous Galerkin methods for the Cahn-Hilliard type equations[J]. J Comput Phys, 2007, 227(1):472-491.
[10] 田明鲁,刘蕴贤.Cahn-Hilliard方程的局部间断Galerkin方法[J]. 山东大学学报(理学版), 2010, 45(8):27-31. TIAN Minglu, LIU Yunxian, The local discontinuous Galerkin method for the Cahn-Hilliard equation[J]. Journal of Shandong University(Natural Science), 2010, 45(8):27-31.
[11] MILLER K, MILLER R N. Moving finite elements(I)[J]. SIAM J Numer Anal, 1981, 18(6):1019-1032.
[12] DVINSKY A S. Adaptive grid generation from harmonic maps on Riemannian manifolds[J]. J Comput Phys, 1991, 95(2):450-476.
[13] HUANG W Z, REN Y H, RUSSELL R D. Moving mesh partial differential equations(MMPDES)based on the equidistribution principle[J]. SIAM J Numer Anal, 1994, 31(3):709-730.
[14] CAO W M, HUANG W Z, RUSSELL R D. An r-adaptive finite element method based upon moving mesh PDEs[J]. J Comput Phys, 1999, 149(2):221-244.
[15] HUANG W Z, RUSSELL R D. Adaptive mesh movement: the MMPDE approach and its applications[J]. J Comput Appl Math, 2001, 128(1/2):383-398.
[16] HUANG W Z, KAMENSKI L. On the mesh nonsingularity of the moving mesh PDE method[J]. Math Comput, 2018, 87:1887-1911.
[17] 杨晓波. 求解双曲守恒律和辐射扩散方程的移动网格方法[D].南京:南京大学, 2013. YANG Xiaobo. Moving mesh methods for solving conservation law and radiation diffusion systems[D]. Nanjing: Nanjing University, 2013.
[18] LU Changna, HUANG Weizhang, QIU Jianxian. Maximum principle in linear finite element approximations of anisotropic diffusion-convection-reaction problems[J]. Numer Math, 2014, 127(3):515-537.
[19] NGO C, HUANG W Z. A study on moving mesh finite element solution of the porous medium equation[J/OL]. J Comput Phys, 2017[2021-09-23]. https://doi.org/10.1016/j.jcp.2016.11.045.
[20] ZHANG Min, HUANG Weizhang, QIU Jianxian. High-order conservative positivity-preserving DG-interpolation for deforming meshes and application to moving mesh DG simulation of radiative transfer[J]. SIAM J Sci Comput, 2020, 42(5):A3109-A3135.
[21] GONZÁLEZ-PINTO S, MONTIJANO J I, PÉREZ-RODRÍGUEZ S. Two-step error estimators for implicit Runge-Kutta methods applied to stiff systems[J]. ACM T Math Software, 2004, 30(1):1-18.
[22] HUANG W Z, RUSSELL R D. Adaptive moving mesh methods[M]. Berlin: Springer Science & Business Media, 2010.
[23] SONG Huailing, SHU Chiwang. Unconditional energy stability analysis of a second order implicit-explicit local discontinuous Galerkin method for the Cahn-Hilliard equation[J]. J Sci Comput, 2017, 73(2):1178-1203.
[1] WANG Ping-li, SHI Dong-yang. Superconvergence analysis and extrapolation of bilinear finite element for Schrödinger equation [J]. JOURNAL OF SHANDONG UNIVERSITY(NATURAL SCIENCE), 2014, 49(10): 66-71.
[2] TIAN Ming-lu, LIU Yun-xian. The local discontiunous Galerkin method for Cahn-Hilliard equation [J]. J4, 2010, 45(8): 27-31.
Viewed
Full text


Abstract

Cited

  Shared   
  Discussed   
No Suggested Reading articles found!