ORIGINAL PAPERS

A Stable FE-FD Method for Anisotropic Parabolic PDEs with Moving Interfaces

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  • 1. School of Civil and Hydraulic Engineering, NingXia University, Yinchuan 750021, Ningxia, China;
    2. School of Mathematics and Computer Science, NingXia Normal University, Guyuan 756000, Ningxia, China;
    3. Department of Mathematics, North Carolina State University, Raleigh, NC 27695-8205, USA;
    4. Departamento de Matemática Aplicada y Estadística, Universidad Politécnica de Cartagena, Cartagena, Spain

Received date: 2022-10-30

  Revised date: 2023-03-25

  Accepted date: 2023-05-01

  Online published: 2023-07-10

Supported by

B. Dong is partially supported by the National Natural Science Foundation of China (Grant No. 12261070) and the Ningxia Key Research and Development Project of China (Grant No. 2022BSB03048). Z. Li is partially supported by the Simons (Grant No. 633724) and by Fundación Séneca grant 21760/IV/22. J. Ruiz is partially supported by the Spanish national research project PID2019-108336GB-I00 and by Fundación Séneca grant 21728/EE/22. (Este trabajo es resultado de las estancias (21760/IV/22) y (21728/EE/22) financiadas por la Fundación Séneca-Agencia de Ciencia y Tecnología de la Región de Murcia con cargo al Programa Regional de Movilidad, Colaboración Internacional e Intercambio de Conocimiento “Jiménez de la Espada”. (Plan de Actuación 2022)).

Abstract

In this paper, a new finite element and finite difference (FE-FD) method has been developed for anisotropic parabolic interface problems with a known moving interface using Cartesian meshes. In the spatial discretization, the standard P1 FE discretization is applied so that the part of the coefficient matrix is symmetric positive definite, while near the interface, the maximum principle preserving immersed interface discretization is applied. In the time discretization, a modified Crank-Nicolson discretization is employed so that the hybrid FE-FD is stable and second order accurate. Correction terms are needed when the interface crosses grid lines. The moving interface is represented by the zero level set of a Lipschitz continuous function. Numerical experiments presented in this paper confirm second order convergence.

Cite this article

Baiying Dong, Zhilin Li, Juan Ruiz-álvarez . A Stable FE-FD Method for Anisotropic Parabolic PDEs with Moving Interfaces[J]. Communications on Applied Mathematics and Computation, 2024 , 6(2) : 992 -1012 . DOI: 10.1007/s42967-023-00281-x

References

[1] Adams, L., Li, Z.: The immersed interface/multigrid methods for interface problems. SIAM J. Sci. Comput. 24, 463-479 (2002). https://doi.org/10.1137/S1064827501389849
[2] Bergmann, S., Albe, K., Flegel, E., Barragan-Yani, D.A., Wagner, B.: Anisotropic solid-liquid interface kinetics in silicon: an atomistically informed phase-field model. Modell. Simul. Mater. Sci. Eng. 25(6), 065015 (2017). https://doi.org/10.1088/1361-651X/aa7862
[3] Braess, D.: Finite Elements: Theory, Fast Solvers, and Applications in Solid Mechanics, 3rd edn. Cambridge University Press, Cambridge (2007)
[4] Brenner, S.C., Scott, L.R.: The Mathematical Theory of Finite Element Methods. Springer, New York (2002)
[5] De Zeeuw, D.: Matrix-dependent prolongations and restrictions in a blackbox multigrid solver. J. Comput. Appl. Math. 33, 1-27 (1990). https://doi.org/10.1016/0377-0427(90)90252-U
[6] Dong, B.Y., Feng, X.F., Li, Z.: An FE-FD method for anisotropic elliptic interface problems. SIAM J. Sci. Comput. 42, B1041-B1066 (2020). https://doi.org/10.1137/19M1291030
[7] Dong, B.Y., Feng, X.F., Li, Z.: An L second order Cartesian method for 3D anisotropic elliptic interface problems. J. Comput. Math. 40, 886-913 (2022). https://doi.org/10.4208/jcm.2103-m2020-0107
[8] Evans, L. C.: Partial Differential Equations. AMS (1998)
[9] He, X., Lin, T., Lin, Y., Zhang, X.: Immersed finite element methods for parabolic equations with moving interface. Numer. Methods Partial Differential Equations 29(2), 619-646 (2013). https://doi.org/10.1002/num.21722
[10] Hou, T., Li, Z., Osher, S., Zhao, H.: A hybrid method for moving interface problems with application to the Hele-Shaw flow. J. Comput. Phys. 134, 236-252 (1997). https://doi.org/10.1006/jcph.1997.5689
[11] Huang, W., Rokhlin, S.I.: Interface waves along an anisotropic imperfect interface between anisotropic solids. J. Nondestruc. Eval. 11, 185-198 (1992). https://doi.org/10.1007/BF00566409
[12] Langer, J.S.: Instabilities and patten formation in crystal growth. Rev. Modern Phys. 52, 1-28 (1980). https://doi.org/10.1103/RevModPhys.52.1
[13] Levitas, V.I., Warren, J.A.: Phase field approach with anisotropic interface energy and interface stresses: large strain formulation. J. Mech. Phy. Solids. 91, 94-125 (2016). https://doi.org/10.1016/j.jmps.2016.02.029
[14] Li, Z.: Immersed interface method for moving interface problems. Numer. Algorithm 14, 269-293 (1997). https://doi.org/10.1023/A:1019173215885
[15] Li, Z., Ito, K.: Maximum principle preserving schemes for interface problems with discontinuous coefficients. SIAM J. Sci. Comput. 23, 1225-1242 (2001). https://doi.org/10.1137/S1064827500370160
[16] Li, Z., Soni, B.: Fast and accurate numerical approaches for Stefan problems and crystal growth. Numer. Heat Transf. B: Fundam. 35, 461-484 (1999). https://doi.org/10.1080/104077999275848
[17] Lin, T., Lin, Y., Zhang, X.: A method of lines based on immersed finite elements for parabolic moving interface problems. Adv. Appl. Math. Mech. 5(4), 548-568 (2013). https://doi.org/10.1017/S2070073300001387
[18] Lin, T., Lin, Y., Zhang, X.: Immersed finite element method of lines for moving interface problems with nonhomogeneous flux jump. Contemp. Math. 586, 257-265 (2013). https://doi.org/10.1090/conm/586/11633
[19] McFadden, G.B., Wheeler, A.A., Braun, R.J., Coriell, S.R., Sekerka, R.F.: Phase-field models for anisotropic interfaces. Phys. Rev. E 48, 2016-2024 (1993). https://doi.org/10.1103/PhysRevE.48.2016
[20] Morton, K.W., Mayers, D.F.: Numerical Solution of Partial Differential Equations. Cambridge Press, Cambridge (1995)
[21] Sethian, J., Straint, J.: Crystal growth and dendritic solidification. J. Comput. Phys. 98, 231-253 (1992). https://doi.org/10.1016/0021-9991(92)90140-T
[22] Schittkowski, K.: QL-quadratic Programming, version 1.5 (1991). https://www.uni-bayreuth.de/departments/math/~kschittkowski/ql.htm
[23] Suo, Z.: Singularities, interfaces and cracks in dissimilar anisotropic media. Proc. R. Soc. A 427, 331-358 (1990)
[24] Tuncel, N. G., Serbest, A. H.: Reflection and refraction by an anisotropic metamaterial slab with diagonal anisotropy. In: 2015 IEEE International Conference on Microwaves, Communications, Antennas and Electronic Systems (COMCAS), Tel Aviv, Israel, 2015, pp. 1-4. IEEE (2015)
[25] Yang, Q., Zhang, X.: Discontinuous Galerkin immersed finite element methods for parabolic interface problems. J. Comput. Appl. Math. 299, 127-139 (2016). https://doi.org/10.1016/j.cam.2015.11.020
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