case 3.1: turbulent flow over a 2d multi-element airfoil 0 ... · uofm 3rd international workshop...

14
Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil Summary of Results Marco Ceze ([email protected]) UofM 3 rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 1/1

Upload: others

Post on 07-Jul-2020

0 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Case 3.1: Turbulent Flow over a 2D Multi-ElementAirfoil

Summary of Results

Marco Ceze ([email protected])

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 1/1

Page 2: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Case description

Objective:Test high-order methods in turbulent flow conditions over a complexgeometry.Stiff discrete system poses a challenge for the nonlinear solver.Outputs of interest are lift and drag.

Flow and boundary conditions:M∞ = 0.2 at α = 16◦.Re = 9 × 106 based on cref = 0.5588, fully turbulent.Adiabatic, no-slip wall at airfoil.Characteristics-based free stream at outer boundary.

Gas properties:γ = 1.4 and Pr = 0.71.Choice of Sutherland’s law or constant viscosity.

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1

Page 3: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Geometry and provided mesh4070 (coasest) quartic quads generated via agglomeration.Sequence of 3 meshes provided in quad and tri formats.Outer boundary located 50 to 100 chord-lengths away from airfoil.Inner and outer geometries provided.

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 3/1

Page 4: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Participants codes and meshesCranfield:

Spalart-Allmaras (Edwards) turbulence model.WENO, 3rd and 5th-order approximations.Roe or HLLC for inviscid flux, centered average for viscousdiscretization.Backward-Euler with 1st-order Jacobian, LU-SGS linear solver.Linear triangular meshes with 1000 chord-lengths farfield distance.Convergence study on sequence of non-nested meshes.Runs performed on single-node, two 8-core Westmere cores (16partitions).

Michigan:Spalart-Allmaras (ICCFD7 version) turbulence model.Metric-based anisotropic, isotropic h, and hp-adaptation.DG, Lagrange basis, full and tensor-product on reference domain.Roe solver for inviscid flux, BR2 for viscous discretization.CPTC, relaxed line-search, with in-house GMRES and line-Jacobipreconditioner.BAMG mesh (metric-based runs), HOW mesh (quad runs).Runs performed on 6 Westmere cores.

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 4/1

Page 5: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Participants codes and meshes

DLR:Spalart-Allmaras (ICCFD7 version) turbulence model.DG, hierarchical polynomial basis on physical space.Roe solver for inviscid flux, BR2 for viscous discretization.Nonlinear h-or-p-multigrid with Backward Euler smoother.SER for CFL evolution.Structured curved meshes with farfield at 50 chords.GMRES with h-or-p-multigrid preconditioner and line-Jacobismoother.2, 4, 8, and 16 partitions.

Stuttgart:Spalart-Allmaras turbulence model.DG, modal basis.HLL solver for inviscid flux, BR2 for viscous discretization.PTC solver with ILU-GMRES linear solver.High-order mesh via projection of normals.Runs performed on 8 cores.

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 5/1

Page 6: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Drag convergence versus DOFs

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 6/1

Page 7: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Drag convergence versus workunits

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 7/1

Page 8: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Lift convergence versus DOFs

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 8/1

Page 9: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Lift convergence versus workunits

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 9/1

Page 10: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Drag convergence versus Work/DOF

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 10/1

Page 11: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Lift convergence versus Work/DOF

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 11/1

Page 12: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Cp distribution

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 12/1

Page 13: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Cf distribution

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 13/1

Page 14: Case 3.1: Turbulent Flow over a 2D Multi-Element Airfoil 0 ... · UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 2/1. Geometry and provided

Conclusions

Smaller workunits spread this time.Different converged outputs are likely due to different domainboundaries.Good agreement between participants for Cp distribution.Some variation on Cf .Adaptivity saves work, error correction helps but not alwaysreliable specially for lift.We would like all to reach constant Work/DOF in our algorithms.

UofM 3rd International Workshop on High-Order CFD Methods, Jan 3-4, Kissimmee, FL, USA C3.1 14/1