Computational Fluid Dynamics: Principles and ApplicationsElsevier, 11 maj 2001 - 460 sidor Computational Fluid Dynamics: Principles and Applications |
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... Artificial Dissipation . . . . . . . . . 95 4.3.2 Flux-Vector Splitting Schemes . . . . . . . . . . . . . . . 98 4.3.3 Flux-Difference Splitting Schemes . . . . . . . . . . . . . 105 4.3.4 Total Variation Diminishing Schemes ...
... Artificial Dissipation . . . . . . . . . 95 4.3.2 Flux-Vector Splitting Schemes . . . . . . . . . . . . . . . 98 4.3.3 Flux-Difference Splitting Schemes . . . . . . . . . . . . . 105 4.3.4 Total Variation Diminishing Schemes ...
Sida xiii
... artificial dissipation : 17, effective binary diffusivity of species m internal energy per unit mass total energy per unit mass Fourier symbol of the time-stepping operator external force vector flux vector flux tensor amplification ...
... artificial dissipation : 17, effective binary diffusivity of species m internal energy per unit mass total energy per unit mass Fourier symbol of the time-stepping operator external force vector flux vector flux tensor amplification ...
Sida 41
... artificial dissipation (because of its similarity to the viscous terms) has to be added for stabilisation. The most widely known implementation is due to Jameson et al. [61]. On structured grids, it is based on a blend of 2nd- and 4th ...
... artificial dissipation (because of its similarity to the viscous terms) has to be added for stabilisation. The most widely known implementation is due to Jameson et al. [61]. On structured grids, it is based on a blend of 2nd- and 4th ...
Sida 95
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Sida 96
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Innehåll
1 | |
5 | |
29 | |
75 | |
Unstructured Finite Volume Schemes | 129 |
Chapter 6 Temporal Discretisation | 181 |
Chapter 7 Turbulence Modelling | 225 |
Chapter 8 Boundary Conditions | 267 |
Chapter 9 Acceleration Techniques | 299 |
Chapter 10 Consistency Accuracy and Stability | 331 |
Chapter 11 Principles of Grid Generation | 353 |
Chapter 12 Description of the Source Codes | 393 |
A Appendix | 401 |
Index | 435 |
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accuracy AIAA Journal AIAA Paper Algorithm applied approach approximation artificial dissipation average boundary conditions boundary layers cell-centred scheme cell-vertex scheme coarse grid coefficients Compressible Flows Computational Physics conservative variables control volume convergence coordinate Delaunay triangulation denotes discretisation scheme domain dummy cells edge eigenvalues employed Euler Equations evaluated explicit face vector farfield finite volume finite volume method flow variables formulation Fourier symbol GMRES governing equations gradients grid cells grid points implementation implicit operator implicit scheme interpolation inviscid Jameson Large Eddy Simulation linear Mach number matrix Mavriplis median-dual scheme methodology Multigrid Method multistage scheme Navier-Stokes Equations nodes obtained Preconditioning problem residual smoothing Reynolds-averaged Navier-Stokes equations second-order Simulation solution Solver source term spatial discretisation splitting schemes structured Subsection surface tensor tetrahedral time-stepping scheme tion turbulence model Turbulent Flows TVD scheme unit normal vector unstructured grids Unstructured Meshes upwind scheme values viscous fluxes wall
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