4.2 Article

A Gradient Discretisation Method for Anisotropic Reaction-Diffusion Models with Applications to the Dynamics of Brain Tumors

Journal

COMPUTATIONAL METHODS IN APPLIED MATHEMATICS
Volume 21, Issue 4, Pages 753-775

Publisher

WALTER DE GRUYTER GMBH
DOI: 10.1515/cmam-2020-0081

Keywords

A Gradient Discretisation Method (GDM); Gradient Schemes; Convergence Analysis; Existence of Weak Solutions; Anisotropic Reaction-Diffusion Models; Dirichlet and Neumann Boundary Conditions; Non-Conforming Finite Element Methods; Finite Volume Schemes; Hybrid Mixed Mimetic (HMM) Method; Non-Conforming P1 Finite Element Scheme; Brain Tumor Dynamics; Fractional Anisotropy

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The paper explores the application of the gradient discretisation method (GDM) in anisotropic reaction-diffusion problems, proving both the existence of weak solutions and the uniform-in-time convergence of the discrete solution and strong convergence of its gradient. It also examines the use of non-conforming numerical schemes on a generic grid.
A gradient discretisation method (GDM) is an abstract setting that designs the unified convergence analysis of several numerical methods for partial differential equations and their corresponding models. In this paper, we study the GDM for anisotropic reaction-diffusion problems, based on a general reaction term, with Neumann boundary condition. With natural regularity assumptions on the exact solution, the framework enables us to provide proof of the existence of weak solutions for the problem, and to obtain a uniformin-time convergence for the discrete solution and a strong convergence for its discrete gradient. It also allows us to apply non-conforming numerical schemes to the model on a generic grid (the non-conforming P1 finite element scheme and the hybrid mixed mimetic (HMM) methods). Numerical experiments using the HMM method are performed to assess the accuracy of the proposed scheme and to study the growth of glioma tumors in heterogeneous brain environment. The dynamics of their highly diffusive nature is also measured using the fraction anisotropic measure. The validity of the HMMis examined further using four different mesh types. The results indicate that the dynamics of the brain tumor is still captured by the HMM scheme, even in the event of a highly heterogeneous anisotropic case performed on the mesh with extreme distortions.

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