2019
DOI: 10.1093/imanum/dry095
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A mixed DG method and an HDG method for incompressible magnetohydrodynamics

Abstract: In this paper we propose and analyze a mixed DG method and an HDG method for the stationary Magnetohydrodynamics (MHD) equations with two types of boundary (or constraint) conditions. The mixed DG method is based on a recent work proposed by Houston et. al. in [25] for the linearized MHD. With two novel discrete Sobolev embedding type estimates for the discontinuous polynomials, we provide a priori error estimates for the method on the nonlinear MHD equations. In the smooth case, we have optimal convergence r… Show more

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Cited by 22 publications
(9 citation statements)
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References 46 publications
(66 reference statements)
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“…The magnetic pressure may be interpreted as a Lagrange multiplier associated with the ∇ • B = 0 condition and, for a suitable choice of boundary conditions, it is identically zero [30]. Inclusion of a magnetic pressure to enforce the ∇ • B = 0 condition is common in both continuous Galerkin [6,9,30,31] and discontinuous Galerkin [21,29,32] finite element methods.…”
Section: Variable Traction Specifications On the Neumann Boundary Hmentioning
confidence: 99%
See 1 more Smart Citation
“…The magnetic pressure may be interpreted as a Lagrange multiplier associated with the ∇ • B = 0 condition and, for a suitable choice of boundary conditions, it is identically zero [30]. Inclusion of a magnetic pressure to enforce the ∇ • B = 0 condition is common in both continuous Galerkin [6,9,30,31] and discontinuous Galerkin [21,29,32] finite element methods.…”
Section: Variable Traction Specifications On the Neumann Boundary Hmentioning
confidence: 99%
“…This requires special treatment of the terms that couple the velocity and magnetic fields to arrive at a method that is energy stable. It should be noted that a previously presented HDG method for the incompressible MHD equations does yield pointwise divergence-free velocity fields [29], but it yields only discretely divergence-free magnetic fields.…”
Section: Introductionmentioning
confidence: 98%
“…for real number j ∈ [1, k +3] and p ∈ H j (Ω). Next, we introduce an interpolation ( [6,29]): for any v ∈ H s (curl; Ω) with s > 1 2 , we define…”
Section: Interpolations For Integer ℓ ≥ 1 We Denote By π Curlmentioning
confidence: 99%
“…There are vast literatures on numerical methods solving the MHD model without the quad-curl term ∇×(∇×(∇×(∇×u))), see [3,10,11,15,19,20,23,29] and references therein for detailed information. However, when the quad-curl term ∇ × (∇ × (∇ × (∇ × u))) is present, the design and analysis of numerical methods for the MHD model becomes more difficult and challenging.…”
Section: Introductionmentioning
confidence: 99%
“…Also in [1,3], the authors have studied the stationary magnetohydrodynamic equations of electrically and heat conducting fluid. For the discretization approaches of (M H D), a few related contributions include mixed finite elements [13,14,16], discontinuous galerkin finite elements [15] or iterative penalty finite element methods [12] and so on. The boundary condition under the form P = P 0 + α i on Γ i , i = 1, .…”
Section: Introductionmentioning
confidence: 99%