A vector penalty-projection approach for the time-dependent incompressible magnetohydrodynamics flows
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Publication:2159906
DOI10.1016/j.camwa.2022.06.019OpenAlexW4283700648WikidataQ114201434 ScholiaQ114201434MaRDI QIDQ2159906
Publication date: 2 August 2022
Published in: Computers \& Mathematics with Applications (Search for Journal in Brave)
Full work available at URL: https://doi.org/10.1016/j.camwa.2022.06.019
Navier-Stokes equations for incompressible viscous fluids (76D05) Stability and convergence of numerical methods for initial value and initial-boundary value problems involving PDEs (65M12) Finite element methods applied to problems in fluid mechanics (76M10) Magnetohydrodynamics and electrohydrodynamics (76W05) Finite element, Rayleigh-Ritz and Galerkin methods for initial value and initial-boundary value problems involving PDEs (65M60)
Related Items (5)
A second-order scheme based on blended BDF for the incompressible MHD system ⋮ A Penalty Finite Element Method for the Stationary Closed-Loop Geothermal Model ⋮ A fully discrete decoupled finite element method for the thermally coupled incompressible magnetohydrodynamic problem ⋮ A sparse grad-div stabilized algorithm for the incompressible magnetohydrodynamics equations ⋮ Error analysis of vector penalty-projection method with second order accuracy for incompressible magnetohydrodynamic system
Cites Work
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- A kinematic vector penalty-projection method for incompressible flow with variable density
- A new fast method to compute saddle-points in constrained optimization and applications
- Convergence results for the vector penalty-projection and two-step artificial compressibility methods
- Stable finite element methods preserving \(\nabla \cdot \boldsymbol{B}=0\) exactly for MHD models
- A fast vector penalty-projection method for incompressible non-homogeneous or multiphase Navier-Stokes problems
- Magnetohydrodynamics. Transl. from the French by A. F. Wright, typeset by C. Philippe
- Convergence analysis of an unconditionally energy stable projection scheme for magneto-hydrodynamic equations
- Second order unconditionally convergent and energy stable linearized scheme for MHD equations
- On an efficient second order backward difference Newton scheme for MHD system
- On the global unique solvability of initial-boundary value problems for the coupled modified Navier-Stokes and Maxwell equations
- Fast discrete Helmholtz-Hodge decompositions in bounded domains
- Two-level defect-correction locally stabilized finite element method for the steady Navier-Stokes equations
- An Oseen scheme for the conduction-convection equations based on a stabilized nonconforming method
- Decoupled schemes for unsteady MHD equations. II: Finite element spatial discretization and numerical implementation
- Fully discrete finite element approximation of the 2D/3D unsteady incompressible magnetohydrodynamic-Voigt regularization flows
- Helicity-conservative finite element discretization for incompressible MHD systems
- A fully decoupled linearized finite element method with second-order temporal accuracy and unconditional energy stability for incompressible MHD equations
- A finite element method for MHD that preserves energy, cross-helicity, magnetic helicity, incompressibility, and \(\operatorname{div} B = 0\)
- The Arrow-Hurwicz iterative finite element method for the stationary thermally coupled incompressible magnetohydrodynamics flow
- Optimal convergence analysis of Crank-Nicolson extrapolation scheme for the three-dimensional incompressible magnetohydrodynamics
- Second order fully decoupled and unconditionally energy-stable finite element algorithm for the incompressible MHD equations
- A decoupled, linear and unconditionally energy stable scheme with finite element discretizations for magneto-hydrodynamic equations
- A modular Grad-div stabilization for the 2D/3D nonstationary incompressible magnetohydrodynamic equations
- Fully decoupled, linear and unconditionally energy stable time discretization scheme for solving the magneto-hydrodynamic equations
- An Introduction to Magnetohydrodynamics
- A subgrid stabilization finite element method for incompressible magnetohydrodynamics
- Unconditionally stable operator splitting algorithms for the incompressible magnetohydrodynamics system discretized by a stabilized finite element formulation based on projections
- Unconditional convergence of the Euler semi-implicit scheme for the 3D incompressible MHD equations
- A Connection Between Scott–Vogelius and Grad-Div Stabilized Taylor–Hood FE Approximations of the Navier–Stokes Equations
- A stabilized Oseen iterative finite element method for stationary conduction-convection equations
- Mathematical Methods for the Magnetohydrodynamics of Liquid Metals
- Numerical analysis of the Crank–Nicolson extrapolation time discrete scheme for magnetohydrodynamics flows
- Finite-Element Approximation of the Nonstationary Navier–Stokes Problem. Part IV: Error Analysis for Second-Order Time Discretization
- Convergent finite element discretizations of the nonstationary incompressible magnetohydrodynamics system
- Finite Element Methods for Navier-Stokes Equations
- Stability and Error Analysis for the First-Order Euler Implicit/Explicit Scheme for the 3D MHD Equations
- A fully divergence-free finite element method for magnetohydrodynamic equations
- Convergence of a vector penalty projection scheme for the Navier Stokes equations with moving body
- On the error estimates of the vector penalty-projection methods: Second-order scheme
- A Preconditioned Semi-Implicit Method for Magnetohydrodynamics Equations
- Vector Penalty-Projection Methods for Open Boundary Conditions with Optimal Second-Order Accuracy
- Unconditional convergence of the Euler semi-implicit scheme for the three-dimensional incompressible MHD equations
- Decoupled schemes for unsteady MHD equations. I. time discretization
- A finite element method for magnetohydrodynamics
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