2020
DOI: 10.1016/j.jcp.2019.108991
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An energy-preserving level set method for multiphase flows

Abstract: The computation of multiphase flows presents a subtle energetic equilibrium between potential (i.e., surface) and kinetic energies. The use of traditional interface-capturing schemes provides no control over such a dynamic balance. In the spirit of the wellknown symmetry-preserving and mimetic schemes, whose physics-compatible discretizations rely upon preserving the underlying mathematical structures of the space, we identify the corresponding structure and propose a new discretization strategy for curvature.… Show more

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Cited by 17 publications
(32 citation statements)
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“…While we succeeded at the formulation of a fully mass conservative and energy-preserving scheme, the conservation of linear momentum is still unclear [16]. However, as it was already commented in [1], while the lack of total momentum conservation is an undesired property, the adoption of an energypreserving scheme provides a bound on total energy and thus stability. Nonetheless, the conservation of linear momentum is an active line of research that deserves further discussion.…”
Section: Discussionmentioning
confidence: 80%
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“…While we succeeded at the formulation of a fully mass conservative and energy-preserving scheme, the conservation of linear momentum is still unclear [16]. However, as it was already commented in [1], while the lack of total momentum conservation is an undesired property, the adoption of an energypreserving scheme provides a bound on total energy and thus stability. Nonetheless, the conservation of linear momentum is an active line of research that deserves further discussion.…”
Section: Discussionmentioning
confidence: 80%
“…We proceed as in [1] by discretizing differential geometry operators from a geometrical perspective and then construct discrete vector calculus operators within a finite volume method. Once we obtain the discrete versions of the differential geometry operators, we construct the discrete counterparts of divergence (D), gradient (G), Laplacian (L) and convective (C(•)) operators, resulting in a classical finite volume, second order, staggered method as introduced by Harlow and Welch [23,13].…”
Section: Discretizationmentioning
confidence: 99%
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“…Let's assume that we use the same staggered formulation in conjunction with a second-order Adams-Bashforth scheme that, for the single phase case, led to the LU decomposition given in Eq.(10). However, for incompressible multiphase flows with interface tracking, density is not constant [15]. This necessarily leads to a modification of the block system of equations.…”
Section: Pressure-velocity Coupling: a Unified Frameworkmentioning
confidence: 99%