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Techniques for High-order Adaptive Discontinuous Galerkin Discretizations in Fluid Dynamics Dissertation Defense

Techniques for High-order Adaptive Discontinuous Galerkin Discretizations in Fluid Dynamics Dissertation Defense Li Wang PhD Candidate Department of Mechanical Engineering University of Wyoming Laramie, WY April 21, 2009 Outline Introduction Objective Steady Flow Problems

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Techniques for High-order Adaptive Discontinuous Galerkin Discretizations in Fluid Dynamics Dissertation Defense

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  1. Techniques for High-order Adaptive Discontinuous Galerkin Discretizations in Fluid DynamicsDissertation Defense Li Wang PhD Candidate Department of Mechanical Engineering University of Wyoming Laramie, WY April 21, 2009

  2. Outline • Introduction • Objective • Steady Flow Problems • High-order Steady-State Discontinuous Galerkin Discretizations • Output-Based Spatial Error Estimation and Mesh Adaptation • Unsteady Flow Problems • High-order Implicit Temporal Discretizations • Output-Based Temporal Error Estimation and Time-step Adaptation • Conclusions and Future Work

  3. Introduction • ComputationalFluid Dynamics (CFD) • Computational methods vs. Experimental methods • Indispensible technology • Inaccuracies and uncertainties • Improvement of numerical algorithms • High-order accurate methods • Sensitivity analysis techniques • Adaptive mesh refinement (AMR) L. Wang, transonic flow over a NACA0012 airfoil with sub-grid shock resolution (2008) M. Nemec, et. cl., Mach number contours around LAV (2008) D. Mavriplis, DLR-F6 Wing-Body Configuration (2006)

  4. Introduction • Why Discontinuous Galerkin (DG) Methods? • Finite difference methods • Simple geometries • Finite volume methods • Lower-order accurate discretizations • DG methods • Solution Expansion • Asymptotic accuracy properties: • Compact element-based stencils • Efficient performance in a parallel environment • Easy implementation of h-p adaptivity

  5. Introduction • High-order Time-integration Schemes • Explicit schemes (e.g. Explicit Runge-Kutta scheme) • Easy to solve • Restricted time-step sizes : • Run a lot of time steps • Implicit schemes • No restriction by CFL stability limit • Accuracy requirement • Accuracy • Computational cost • Efficient Solution Strategies • Required for steady-state or time-implicit solvers • p- or hp- nonlinear multigrid approach • Element Jacobi smoothers

  6. Introduction • Sensitivity Analysis Techniques • Applications • Shape optimization • Output-based error estimation • Adaptive mesh refinement • Adjoint Methods • Linearization of the analysis problem + Transpose • Discrete adjoint method • Reproduce exact sensitivities to the discrete system • Deliver Linear systems • Simulation output : L(u), such as lift or drag • Error in simulation output: e(L) ~ (Adjoint solution) • (Residual of the Analysis Problem)

  7. Objective • Development of Efficient Solution Strategies for Steady or Unsteady Flows • Development of Output-based Spatial Error Estimation and Mesh Adaptation • Investigation of Time-Implicit Schemes • Investigation of Output-based Temporal Error Estimation and Time-Step Adaptation

  8. Model Problem • Two-dimensional Compressible Euler Equations • Conservative Formulation

  9. Outline • Introduction • Objective • Steady Flow Problems • High-order Steady-State Discontinuous Galerkin Discretizations • Output-Based Spatial Error Estimation and Mesh Adaptation • Unsteady Flow Problems • High-order Implicit Temporal Discretizations • Output-Based Temporal Error Estimation and Time-step Adaptation • Conclusions and Future Work

  10. Discontinuous Galerkin Discretizations • Triangulation Partition: • DG weak statement on each element, k • Integrating by parts • Solution Expansion • Steady-state system of equations

  11. Compressible Channel Flow over a Gaussian Bump • Free stream Mach number = 0.35 • HLLC Riemann flux approximation • Mesh size: 1248 elements Pressure contours usingp=0discretization and p=0 boundary elements Pressure contours using p=4 discretization and p=4 boundary elements

  12. Compressible Channel Flow over a Gaussian Bump • Spatial Accuracy and Efficiency for Various Discretization Orders Error convergence vs. Grid spacing Error convergence vs. Computational time

  13. Compressible Channel Flow over a Gaussian Bump • Element Jacobi Smoothers • Single level method • p-independent • h-dependent

  14. Compressible Channel Flow over a Gaussian Bump • p- or hp-multigrid approach • p-independent • h-independent

  15. Outline • Introduction • Objective • Steady Flow Problems • High-order Steady-State Discontinuous Galerkin Discretizations • Output-Based Spatial Error Estimation and Mesh Adaptation • Unsteady Flow Problems • High-order Implicit Temporal Discretizations • Output-Based Temporal Error Estimation and Time-step Adaptation • Conclusions and Future Work

  16. Output-based Spatial Error Estimation • Some key functional outputs in flow simulations • Lift, Drag, Integrated surface temperature, etc. • Surface integrals of the flow-field variables • Single objective functional, L • Coarse affordable mesh, H • Coarse level flow solution, • Coarse level functional, • Fine (Globally refined) mesh, h • Fine level flow solution, • Fine level functional, • Goal: Find an approximation of without solving on the fine mesh

  17. Output-based Spatial Error Estimation • Taylor series expansion • Goal: Find an approximation of without solving on the fine mesh

  18. Output-based Spatial Error Estimation • Discrete adjoint problem (H) • Transpose of Jacobian matrix • Delivers similar convergence rate as the flow solver • Reconstruction of coarse level adjoint • : Estimates functional error • : Indicates error distribution and drives mesh adaptation • Approximated fine level functional

  19. Refinement Criteria • is used to drive mesh adaptation • Element-wise error indicator • Set an error tolerance, ETOL • Necessary refinement for an element if • Flag elements required for refinement

  20. P P p p+1 P P h H H Mesh Refinement • h-refinement • Local mesh subdivision • p-enrichment • Local variation of discretization orders • hp-refinement • Local implementation of the h- orp-refinement individually

  21. Additional Criteria for hp-refinement • For each flagged element: • How to make a decision between h- and p-refinement? Smoothness indicator • Local smoothness indicator • Element-based Resolution indicator[Persson, Peraire] • Inter-element Jump indicator [Krivodonova,Xin,Chevaugeon,Flaherty],

  22. Subsonic Flow over a Four-Element Airfoil • Free-stream Mach number = 0.2 • Various adaptation algorithms • h-refinement • p-enrichment • Objective functional: drag or lift (angle of attack = 0 degree) • Starting interpolation order of p = 1 • HLLC Riemann solver • hp-Multigrid accelerator Initial mesh (1508 elements)

  23. Subsonic Flow over a Four-Element Airfoil Mach number contours Flow and adjoint problems target functional of lift Adjoint solution, Λ(2) Comparisons on hp-Multigrid convergence for the flow and adjoint solutions

  24. h-Refinement for Target Functional of Lift • Fixed discretization order of p = 1 Final h-adapted mesh (8387 elements) Close-up view of the final h-adapted mesh

  25. h-Refinement for Target Functional of Lift • Comparison between h-refinement and uniform mesh refinement Error convergence history vs. degrees of freedom Error convergence history vs. CPU time (sec)

  26. p-Enrichment for Target Functional of Drag • Fixed underlying grids (1508 elements) Spatial error distribution for the objective functional of drag Final p-adapted mesh discretization orders: p=1~4

  27. p-Enrichment for Target Functional of Drag • Comparison between p-enrichment and uniform order refinement Error convergence history vs. CPU time (sec) Error convergence history vs. degrees of freedom

  28. Hypersonic Flow over a half-circular Cylinder • Free-stream Mach number of 6 • Objective functional: surface integrated temperature, • hp-refinement • Starting discretization order of p=0 (first-order accurate) • hp-adapted meshes Final hp-adapted mesh: 42,234 elements. Discretization orders: p=0~3 Initial mesh: 17,072 elements

  29. Hypersonic Flow over a half-circular Cylinder • Final pressure and Mach number solutions

  30. Hypersonic Flow over a half-circular Cylinder • Convergence of the objective functional

  31. Outline • Introduction • Objective • Steady Flow Problems • High-order Steady-State Discontinuous Galerkin Discretizations • Output-Based Spatial Error Estimation and Mesh Adaptation • Unsteady Flow Problems • High-order Implicit Temporal Discretizations • Output-Based Temporal Error Estimation and Time-step Adaptation • Conclusions and Future Work

  32. Implicit Time-integration Schemes • Time-Implicit System • First-orderaccurate backwards difference scheme (BDF1) • Second-order accurate multistep backwards difference scheme (BDF2) • Second-order Crank Nicholson scheme (CN2) • Fourth-order implicit Runge-Kutta scheme (IRK4)

  33. Convection of an Isentropic Vortex • Initial condition • Isentropic vortex perturbation; Periodic boundary conditions • HLLC Flux approximation • p = 4 spatial discretization • ∆ t = 0.2 BDF1 (First-order accurate) IRK4 (Fourth-order accurate)

  34. Convection of an Isentropic Vortex • Temporal accuracy and efficiency study for various temporal schemes Error convergence vs. time-step sizes Error convergence vs. Computational time

  35. Shedding Flow over a Triangular Wedge • Free-stream Mach number = 0.2 • Unstructured mesh with 10836 elements • Various spatial discretizations and temporal schemes Unstructured computational mesh with 10836 elements

  36. Shedding Flow over a Triangular Wedge • Free-stream Mach number = 0.2 • Unstructured mesh with 10836 elements • Various spatial discretizations and temporal schemes Density solution using p = 1 discretization and BDF2 scheme

  37. Shedding Flow over a Triangular Wedge • t = 100 • Various spatial discretizations and temporal schemes p = 1 and BDF2 p = 1 and IRK4

  38. Shedding Flow over a Triangular Wedge • t = 100 • Various spatial discretizations and temporal schemes p = 1 and BDF2 p = 3 and IRK4

  39. Outline • Introduction • Objective • Steady Flow Problems • High-order Steady-State Discontinuous Galerkin Discretizations • Output-Based Spatial Error Estimation and Mesh Adaptation • Unsteady Flow Problems • High-order Implicit Temporal Discretizations • Output-Based Temporal Error Estimation and Time-step Adaptation • Conclusions and Future Work

  40. Output-based Temporal Error Estimation • Same methodology can be applied in time • Global temporal error estimation and time-step adaptation • Implementation to BDF1 and IRK4 schemes • Time-integrated objective functional: • UnsteadyFlow solution • Unsteady adjoint solution • Linearization of the unsteady flow equations • Transpose operation results in a backward time-integration Forward time-integration Current Backward time-integration

  41. Output-based Temporal Error Estimation • Two successively refined time-resolution levels • H: coarse level functional • h: fine level functional • Approximation of fine level functional BDF1: • Localized functional error (for each time step i) IRK4: • Local time-step subdivision if

  42. Shedding Flow over a Triangular Wedge • Implementation for BDF1 scheme ( p = 2) • Validation of adjoint-based error correction • Objective function: Drag at t = 5 • Error prediction for two time-resolution levels Refined time-resolution levels Computed functional error (Reconstructed adjoint) • (Unsteady residual)

  43. Shedding Flow over a Triangular Wedge • Adaptive time-step refinement approach vs. Uniform time-step refinement approach • Objective functional: Error convergence vs. time steps (i.e. DOF) Error convergence vs. computational cost

  44. Outline • Introduction • Objective • Steady Flow Problems • High-order Steady-State Discontinuous Galerkin Discretizations • Output-Based Spatial Error Estimation and Mesh Adaptation • Unsteady Flow Problems • High-order Implicit Temporal Discretizations • Output-Based Temporal Error Estimation and Time-step Adaptation • Conclusions and Future Work

  45. Conclusions • High-order DG and Implicit-Time Methods • Optimal error convergence rates are attained for the DG discretizations • Perform more efficiently than lower-order methods • Both h- and p-independent convergence rates • An attempt to balance spatial and temporal error • Perform more efficiently than lower-order implicit temporal schemes • h-independent convergence rates and slightly dependent on time-step sizes • Discrete Adjoint based Sensitivity Analysis • Formulation of discrete adjoint sensitivity for DG discretizations • Accurate error estimate in a simulation output • Superior efficiency over uniform mesh or order refinement approach • hp-adaptation shows good capturing of strong shocks without limiters • Extension to temporal schemes • Superior efficiency over uniform time-step refinement approach

  46. Future Work • Dynamic Mesh Motion Problems • Discretely conservative high-order DG • Both high-order temporal and spatial accuracy • Unsteady shape optimization problems with mesh motion • Robustness of the hp-adaptive refinement strategy • Incorporation of a shock limiter • Investigation of smoothness indicators • Combination of spatial and temporal error estimation • Quantification of dominated error source • More effective adaptation strategies • Extension to other sets of equations • Compressible Navier-Stokes equations (IP method) • Three-dimensional problems

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