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Finite-Volumes I Sauro Succi
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Finite Volumes Real-life geometries: coordinate-free Courtesy of Prof. M. Porfiri, NYU Poly
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Given a Volume V, enclosed in a piecewise smooth boundary (surface) S, characterized by the normal n in each point; The flux of a is defined as IF S is regular and a is continuously differentiable, we have the following: Gauss theorem
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Gauss theorem: conservation laws
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Volume vs Surface average
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Gauss theorem: ADE
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Gauss theorem: Control Volume
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Conservativeness
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Colocated; Control Volume Simple, but not good for surfint > geos VP uncoupled, hourglass N E W S e n s w ne
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Centers to Edges: Interpolate E e n s w ne N
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Staggered Laborious, no interpolation > simple geos No hourglass, VP coupled
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Discretized Gauss: Continuity Discretized Fluxes: Interpolation
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Discretized Fluxes: General Discretized Fluxes: Interpolation
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Finite Volumes
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Topological issues
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FD<FV<FE Cartesian Non-Cartesian, Structured Unstructured
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1d and 2d example: advection-diffusion
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FV: AD d=2 Discretized Fluxes
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One Dimension
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Linear Interp: Upwind:
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One Dimension
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1d: example Give explicit expression of L_PQ and show that it reduces to standard FD for square finite volumes. Again, we don’t care about non-uniformity because the unknowns are cell averages (more physical)
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Two-dimensions
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Going to 2D: same principles more labour! Cartesian (Orthogonal) Trapezoidal (non-orthogonal) Unstructured (similar to FEM)
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d d d d Cartesian d=2
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Structured cartesian: Advection fluxes
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Structured cartesian: diffusive flux Structured matrix: 5 nonzero entries
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Structured cartesian: Advection fluxes
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2d cartesian: diffusive fluxes
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Structured cartesian: cieff’s Structured matrix: 5 nonzero entries
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Structured non-cartesian
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Structured Non-Cartesian Geometrical data
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CEV = Centers/Edges/Vertices Non-cartesian: structured S W N Ε NΕ SΕ NW SW ne se C ew n s Non-orthogonal Still structured
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Co/Contravariant/Cartesian
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CEV = Centers/Edges/Vertices Staggered S W N Ε NΕ SΕ NW SW ne se C ew n s Non-orthogonal
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Navier-Stokes (Compressible) Staggered FV
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NW NΕ SΕ SW n e w s P E N W S Vertex-centered staggered
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Discretized Gauss: Continuity Discretized Convective Fluxes Same for north,west, south … Non-orthogonality issues (!) S W N Ε NΕ SΕ NW SW ne se C ew n s
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Discretized Gauss: Continuity Discretized midpoint (2 nd order 8 neigh) Discretized Simpson (4 th order, 8 neigh)
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Discretized Convective Fluxes
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Discretized Gauss: Momentum_x Convective and Dissipative Fluxes
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Non-Linear (outer) iteration Nonlinear (outer) iteration, k=0,1…
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Real-life geometries Courtesy of Prof. M. Porfiri, NYU Poly
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Example: Global: Cylindrical, Spherical, Local: Oblique
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Unstructured FV~FEM
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Cell vs Vertex Centered
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Vertex control elements
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Finite Volumes: summary Intuitive and physically sound Round-off Conservative (fluxin=-fluxout) Geo-topological ahead, laborious Interpolation to be decided (unlike FEM) Structured: Finite-Difference with non-smooth coordinates No-singularity (1/r for sherical coordinates) Commercially dominant (STAR-CD, FLUENT…)
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