2020
DOI: 10.1016/j.jcp.2020.109439
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A conservative finite element method for the incompressible Euler equations with variable density

Abstract: We construct a finite element discretization and time-stepping scheme for the incompressible Euler equations with variable density that exactly preserves total mass, total squared density, total energy, and pointwise incompressibility. The method uses Raviart-Thomas or Brezzi-Douglas-Marini finite elements to approximate the velocity and discontinuous polynomials to approximate the density and pressure. To achieve exact preservation of the aforementioned conserved quantities, we exploit a seldom-used weak form… Show more

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Cited by 20 publications
(14 citation statements)
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“…For example, the stream function / vorticity formulation, which proved particular effective in 2D, does not exist in the same simple form there. One alternative would be to use a structure preserving discretization of the Navier-Stokes equations, e.g., [20,21], as a basis. The built-in constraints, such as an inherently divergence-free velocity vector field, would then again aid the physicality of the learned solution and simplify the learning task.…”
Section: Discussionmentioning
confidence: 99%
“…For example, the stream function / vorticity formulation, which proved particular effective in 2D, does not exist in the same simple form there. One alternative would be to use a structure preserving discretization of the Navier-Stokes equations, e.g., [20,21], as a basis. The built-in constraints, such as an inherently divergence-free velocity vector field, would then again aid the physicality of the learned solution and simplify the learning task.…”
Section: Discussionmentioning
confidence: 99%
“…As a consequence of the symmetry (12), one can associate to L the Lagrangian (u, ρ) in Eulerian form, as follows…”
Section: Compressible Flowsmentioning
confidence: 99%
“…In particular the discretization corresponds to a weak form of the compressible fluid equation that doesn't seem to have been used in the finite element literature. An incompressible version of this expression of the weak form has been used in [12] for the incompressible fluid with variable density. The setting that we develop applies in general to 2D and 3D fluid models that can be written in Euler-Poincaré form.…”
Section: Introductionmentioning
confidence: 99%
“…The approach we develop in this paper is built on our earlier work on conservative methods for compressible fluids (Gawlik & Gay-Balmaz 2020b) and for incompressible MHD with variable density in Gawlik & Gay-Balmaz (2020a. Two notable differences that arise in the viscous, resistive compressible setting are the change in boundary conditions for the velocity and magnetic fields, and the fact that the magnetic field is not advected as a vector field when the fluid is compressible; that is, curl(B × u) does not coincide with the Lie derivative of the vector field B along u when divu = 0.…”
Section: Introductionmentioning
confidence: 99%