2012
DOI: 10.1007/978-94-007-4038-9_7
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Algebraic Flux Correction II

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Cited by 35 publications
(43 citation statements)
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“…In the former equation U = (ρ, ρu, ρv, ρE) T = (U (1) , U (2) , U (3) , U (4) ) is the vector of conservative variables. The effective density is given by ρ = α p ρ p , and v = (u, v) T denotes the velocity vector.…”
Section: Mathematical Propertiesmentioning
confidence: 99%
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“…In the former equation U = (ρ, ρu, ρv, ρE) T = (U (1) , U (2) , U (3) , U (4) ) is the vector of conservative variables. The effective density is given by ρ = α p ρ p , and v = (u, v) T denotes the velocity vector.…”
Section: Mathematical Propertiesmentioning
confidence: 99%
“…Hyperbolic solvers can be applied to the equations governing the gas phase, while scalar dissipation is feasible for the pressureless conservation laws of the particulate phase. The design of the artificial diffusion operator for the gas phase can be found in [4,2,9,18]. Therefore it remains to define the stabilization of the particulate phase.…”
Section: Discretizationmentioning
confidence: 99%
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“…Therefore, it is hard to impose the Dirichlet boundary conditions in the usual way. It is common practice to recover the boundary values by switching to the characteristic variables, evaluating the incoming Riemann invariants from the physical boundary conditions and extrapolating the outgoing ones from the interior of the computational domain (Kuzmin & Möller, 2004).…”
Section: Boundary Conditionsmentioning
confidence: 99%