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1 On forward in time differencing: an unstructured mesh framework Joanna Szmelter Piotr Smolarkiewicz Loughborough University NCAR UK Colorado USA
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2 Edge based data Finite Volume ( Smolarkiewicz, Szmelter JCP 2005 ) 2D3D
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3 Edge based data structure ☺ Flexible mesh adaptivity and hybrid meshes ☺ Low storage ☺ Easy generalisation to 3D, vectorisation, parallelisation, mesh agglomeration ☺ Less expensive than element based data structure More expensive operations than I,J,K
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Notion of the edge-based MPDATA: ADVECTION FIRST ORDER UPWIND (DONOR CELL) compensating velocity
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MPDATA BASIC SCHEME ITERATED UPWIND FIRST ORDER UPWIND
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6 Structured v Unstructured
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7 CONVERGENCE OF FINITE-VOLUME MPDATA ON UNSTRUCTURED MESH
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8 CONVERGENCE OF FINITE-VOLUME MPDATA ON UNSTRUCTURED SKEWED MESH
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9 REVOLUTION OF A SPHERE AROUND THE DIAGONAL OF A DOMAIN INITIAL MPDATA GAGE AFTER 1 REVOLUTION
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NFT MPDATA: a general template implicit integration preconditioned non-symmetric Krylov-subspace elliptic solver explicit integration
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11 Compressible flows Explicit integration (Smolarkiewicz, Szmelter JCP 2008 published on line)
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Classical Total Energy Equation Modified Total Energy Equation Potential Temperature Equation Internal Energy Equation
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13 M = 5 M = 15 M =2. 5 Supersonic flows Mesh adaptivity by remeshing
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14 ADAPTIVITY with a refinement indicator based on MPDATA lead error (Szmelter,Smolarkiewicz IJNMF 2005) Mesh movement Point enrichment
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15 Transonic flow NACA012 M=0.85 α=1.25º MPDATARunge-Kutta
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16 CONVERGENCE STUDY MPDATA - NFT EULER SOLVER M=0.5 MPDATA UPWIND
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17 Flow past a cylinder M=0.38
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18 Flow past a cylinder M=0.38 --- Entropy deviation triangular meshes Potential temperature Internal energy Total energy Modified total energy
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20 3D Spherical wave; Analytical solution --- Landau & Lifshitz M=0
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21 Incompressible flows Implicit integration
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22 Incompressible flows Re=200. Re=100. Strouhal number =163 Strouhal number =183
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23 Incompressible flows --- multi-connected domains Re=100
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24 2D – non-hydrostatic model Incompressible Boussinesq ILES Orographically forced atmospheric gravity waves vertical wave propagation wave breaking
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25 Flows on a Sphere --- Geospherical coordinates
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26 Shallow water equations initial
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27 Shallow water equations
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28 Shallow water equations Zonal flow over a cone
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29 Potential for modelling of multi-connected domains and easy implementation of mesh adaptivity. (David Parkinson) ( Treatment of hanging nodes & hybrid meshes Szmelter et al Comp. Meth. Appl. Mech. Eng 92)
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30 CONCLUSIONS Presented work opens avenues to construct a flexible edge-based clone of EULAG and to study unstructured meshes performance for all-scale atmospheric flows. Main new effort lies in mesh generation, visualisation and parallelisation.
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