2021
DOI: 10.1016/j.apnum.2021.05.021
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A weak Galerkin finite element method for time fractional reaction-diffusion-convection problems with variable coefficients

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Cited by 28 publications
(5 citation statements)
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“…The key feature of this method is that the classical derivative is replaced by weak derivative in the corresponding variational formulation in a way that completely discontinuous functions have been allowed to use in the numerical scheme which has a parameter independent stabilizer. The weak Galerkin method has been studied and applied to a variety of problems including Stokes equations [32], interface problem [18], Maxwell equation [19], fractional time convection-diffusion problems [28], and singularly perturbed elliptic equations in one and higher dimensions [10,29,30].…”
Section: Introductionmentioning
confidence: 99%
“…The key feature of this method is that the classical derivative is replaced by weak derivative in the corresponding variational formulation in a way that completely discontinuous functions have been allowed to use in the numerical scheme which has a parameter independent stabilizer. The weak Galerkin method has been studied and applied to a variety of problems including Stokes equations [32], interface problem [18], Maxwell equation [19], fractional time convection-diffusion problems [28], and singularly perturbed elliptic equations in one and higher dimensions [10,29,30].…”
Section: Introductionmentioning
confidence: 99%
“…They pointed out that their schemes are well-suited to time FPDEs since they preserve the singularity of the solution. Toprakseven ( 2021 ) utilized the classical L1 discretization in time and a weak Galerkin element in space to establish a weak Galerkin finite element method for the d -dimensional ( ) TFADRE. Kumar and Zeidan ( 2021 ) scrutinized the one-dimensional non-linear TFADRE in which the fractional temporal derivative is defined in the Atangana-Baleanu sense.…”
Section: Introductionmentioning
confidence: 99%
“…The weak functions in WG-FEMs consist of the form u = {u 0 , u b } with u = u 0 inside of the element and u = u b on the boundary of the element. Later on, WG finite element methods have further been presented for a large variety of PDEs including the implementation results [21], parabolic problems [16], the Helmholtz equations with high wave numbers in [22] and the time fractional reaction-diffusion-convection problems in [27]. The weak gradient and weak divergence operators have been introduced for convection-dominated problems in [5] and [17].…”
Section: Introductionmentioning
confidence: 99%