2019
DOI: 10.1016/j.cam.2018.08.023
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An immersed weak Galerkin method for elliptic interface problems

Abstract: In this paper, we present an immersed weak Galerkin method for solving second-order elliptic interface problems. The proposed method does not require the meshes to be aligned with the interface. Consequently, uniform Cartesian meshes can be used for nontrivial interfacial geometry. We show the existence and uniqueness of the numerical algorithm, and prove the error estimates for the energy norm. Numerical results are reported to demonstrate the performance of the method.

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Cited by 13 publications
(2 citation statements)
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“…Concerning the discretization methods for conjugate heat transfer problems (often referred to as elliptic interface problems), a comprehensive literature can be found including finite difference methods, 21,22 finite element methods, [23][24][25] discontinuous Galerkin methods, 26 finite volume methods, [27][28][29][30] lattice Boltzmann methods, 31,32 among others. Finite volume methods are particularly interesting in the context of heat and mass transfer problems, given the conservation property intrinsically preserved and the ease of handling general unstructured meshes.…”
Section: Conjugate Heat Transfer Modelingmentioning
confidence: 99%
“…Concerning the discretization methods for conjugate heat transfer problems (often referred to as elliptic interface problems), a comprehensive literature can be found including finite difference methods, 21,22 finite element methods, [23][24][25] discontinuous Galerkin methods, 26 finite volume methods, [27][28][29][30] lattice Boltzmann methods, 31,32 among others. Finite volume methods are particularly interesting in the context of heat and mass transfer problems, given the conservation property intrinsically preserved and the ease of handling general unstructured meshes.…”
Section: Conjugate Heat Transfer Modelingmentioning
confidence: 99%
“…Furthermore, it is known that WG schemes are absolutely stable, and the corresponding solutions generally preserve the physical quantities inherited by the modeling equations at discrete levels. WG-FEM has been developed for many PDEs including the linear elasticity equation [33], the Stokes equation [44], Maxwell's equation [22,29], the elliptic interface problem [23], the Brinkman equation [17], the Helmholtz equation [24], the Sobolev equation [8], and the wave equation [11] etc. The latest development of WG-FEM is the primal-dual weak Galerkin finite element method for second order elliptic equations in non-divergence form [31] and the Fokker-Planck equation [32].…”
mentioning
confidence: 99%