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Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 1 Application of a Hybrid Navier-Stokes Solver with Automatic.

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Presentation on theme: "Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 1 Application of a Hybrid Navier-Stokes Solver with Automatic."— Presentation transcript:

1 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 1 Application of a Hybrid Navier-Stokes Solver with Automatic Transition Prediction Andreas Krumbein German Aerospace Center, Institute of Aerodynamics and Flow Technology, Numerical Methods Normann Krimmelbein Technical University of Braunschweig, Institute of Fluid Mechanics, Aerodynamics of Aircraft Géza Schrauf Airbus

2 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 2 Outline Introduction Transition Prescription Transition Prediction Coupling Structure Test Cases & Computational Results 2D two-element configuration 3D generic aircraft configuration Conclusion & Outlook

3 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 3 Introduction Background of considering transition in RANS-based CFD tools Better numerical simulation results Capturing of physical phenomena, which were discounted otherwise Quantitatively, sometimes even qualitatively the results can differ significantly w/o transition Long term requirement from research organisations and industry Transition prescription Some kind of transitional flow modelling Transition prediction Automatically: no intervention by the code user Autonomously: as little additional information as possible Main objectives of the functionality Improved simulation of interaction between transition and separation Exploitation of the full potential of advanced turbulence models Objectives of the paper Demonstration of the capabilities using different application modes Documentation for future production application in industry

4 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 4 Different prediction approaches: Empirical/semi-empirical transition criteria for some mechanisms the only thing available, cheap, can be inaccurate Local, linear stability theory + e N method state-of-the-art method in engineering, relatively cheap, relatively accurate Parabolic stability equations (PSE) non-local, linear&non-linear, rather expensive, very accurate, initial conditions: ? Large eddy simulation (LES) unsteady, can be very accurate, not yet mature, very expensive Direct numerical simulation (DNS) of Navier-Stokes equations unsteady, high end approach, nothing is more accurate, unaffordable Introduction

5 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 5 Different prediction approaches: Empirical/semi-empirical transition criteria for some mechanisms the only thing available, cheap, can be inaccurate Local, linear stability theory + e N method state-of-the-art method in engineering, relatively cheap, relatively accurate Parabolic stability equations (PSE) non-local, linear&non-linear, rather expensive, very accurate, initial conditions: ? Large eddy simulation (LES) unsteady, can be very accurate, not yet mature, very expensive Direct numerical simulation (DNS) of Navier-Stokes equations unsteady, high end approach, nothing is more accurate, unaffordable  2  1 Introduction

6 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 6 Different coupling approaches: RANS solver+ stability code + e N method RANS solver+ boundary layer code + stability code + e N method RANS solver+ boundary layer code + e N database method(s) RANS solver+ transition closure model or transition/turbulence model Introduction

7 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 7 Different coupling approaches: RANS solver+ stability code + e N method RANS solver+ boundary layer code + stability code + e N method RANS solver+ boundary layer code + e N database method(s) RANS solver+ transition closure model or transition/turbulence model Introduction

8 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 8 Different coupling approaches: RANS solver+ stability code + e N method RANS solver+ boundary layer code + fully automated stability code + e N method RANS solver+ boundary layer code + e N database method(s) RANS solver+ transition closure model or transition/turbulence model Introduction

9 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 9 Different coupling approaches: RANS solver+ fully automated stability code + e N method RANS solver+ boundary layer code + fully automated stability code + e N method RANS solver+ boundary layer code + e N database method(s) RANS solver+ transition closure model or transition/turbulence model  2  1  3  future Introduction

10 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 10 Hybrid RANS solver TAU: 3D RANS, compressible, steady/unsteady Hybrid unstructured grids: hexahedra, tetrahedra, pyramids, prisms Finite volume formulation Vertex-centered spatial scheme (edge-based dual-cell approach) 2 nd order central scheme, scalar or matrix artifical dissipation Time integration:explicit Runge-Kutta with multi-grid acceleration or implicit approximate factorization scheme (LU-SGS) Turbulence models and approaches: Linear and non-linear 1- and 2-equation eddy viscosity models (SA type, k-  type) RSM  RST, EARSMs (full & linearized) DES Introduction

11 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 11 Transition Prescription Prescription - d lam, main = 20%chord length - d lam, flap = 1%chord length P T upp (main) P T low (flap) P T upp (flap) P T low (main) -automatic partitioning of flow field into laminar and turbulent regions -individual laminar zone for each element -different numerical treatment of laminar and turbulent grid points in laminar regions:  control of TM’s source terms  S prod ≤ 0  S prod : source of turbulence production equation

12 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 12 Transition Prescription Prescription - d lam, main = 20%chord length - d lam, flap = 1%chord length P T upp (main) P T low (flap) P T upp (flap) P T low (main) -automatic partitioning of flow field into laminar and turbulent regions -individual laminar zone for each element -different numerical treatment of laminar and turbulent grid points in laminar regions:  control of TM’s source terms  S prod ≤ 0  S prod : source of turbulence production equation

13 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 13 Transition Prescription Prescription -automatic partitioning of flow field into laminar and turbulent regions -individual laminar zone for each element -different numerical treatment of laminar and turbulent grid points in laminar regions:  control of TM’s source terms  S prod ≤ 0  S prod : source of turbulence production equation - d lam, main = 20%chord length - d lam, flap = 1%chord length P T upp (main) P T low (flap) P T upp (flap) P T low (main)

14 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 14 Transition Prescription Prescription -automatic partitioning of flow field into laminar and turbulent regions -individual laminar zone for each element -different numerical treatment of laminar and turbulent grid points in laminar regions:  control of TM’s source terms  S prod ≤ 0  S prod : source of turbulence production equation - d lam, main = 20%chord length - d lam, flap = 1%chord length P T upp (main) P T low (flap) P T upp (flap) P T low (main)

15 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 15 Structure cycle = k cyc external BL approach Transition Prediction Coupling Structure

16 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 16 cycle = k cyc Structure external BL approach internal BL approach Transition Prediction Coupling Structure

17 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 17 Transition prediction module Structure transition module line-in-flight cuts or inviscid stream lines c p -extraction or lam. BL data from RANS grid lam. BL code swept, tapered  conical flow, 2.5d streamline-oriented external code local lin. stability code e N method for TS & CF external code or e N database methods one for TS & one for CF external codes

18 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 18 Transition prediction module Structure transition module line-in-flight cuts or inviscid stream lines c p -extraction or lam. BL data from RANS grid lam. BL code swept, tapered  conical flow, 2.5d streamline-oriented external code local lin. stability code e N method for TS & CF external code or e N database methods one for TS & one for CF external codes RANS infrastructure

19 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 19 Structure Application areas 2d airfoil configurations 2.5d wing configurations: inf. swept 3d wing configurations 3d fuselages 3d nacelles Single-element configurations Mulit-element configurations Flow topologies attached with lam. separation: - LS point as transition point - bubble with criterion OR real stability analysis with stability code inside bubble + many points in prismatic layer

20 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 20 Structure Application areas 2d airfoil configurations 2.5d wing configurations: inf. swept 3d wing configurations 3d fuselages 3d nacelles Single-element configurations Mulit-element configurations Flow topologies attached with lam. separation: - LS point as transition point - bubble with criterion OR real stability analysis with stability code inside bubble + many points in prismatic layer streamlines necessary! lam. BL data from RANS grid needed! for 3d case: for CF  128 points in wall normal direction necessary!!!

21 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 21 set s tr u and s tr l far downstream (  start mit quasi fully-laminar conditions) compute flow field check for lam. separation in RANS grid  set laminar separation points as new s tr u,l  stabilization of the computation in the transient phase c l  const. in cycles  call transition module  usea.) new transition point directly or b.) lam. separation point of BL code as approximation see new s tr u,l underrelaxed  s tr u,l = s tr u,l , 1.0 <  < 1.5  damping of oscillations in transition point iteration Structure Algorithm

22 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 22 set s tr u and s tr l far downstream (  start mit quasi fully-laminar conditions) compute flow field check for lam. separation in RANS grid  set laminar separation points as new s tr u,l  stabilization of the computation in the transient phase c l  const. in cycles  call transition module  usea.) new transition point directly or b.) lam. separation point of BL code as approximation see new s tr u,l underrelaxed  s tr u,l = s tr u,l , 1.0 <  < 1.5  damping of oscillations in transition point iteration check convergence   s tr u,l <  noyes STOP Structure Algorithm

23 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 23 NLR 7301 with flap gap: 2.6% c main, c flap /c main = 0.34 M = 0.185, Re = 1.35 x 10 6,  = 6.0° grid: 23,000 triangles + 15,000 quadriliterals on contour: main  250, flap  180, 36 in both prismatic layers SAE N TS = 9.0 (arbitrary setting) exp. transition locations: upper  main: 3.5% & flap: 66.5% lower  main: 62.5% & flap: fully laminar different mode combinations: a)laminar BL code& stability code  BL mode 1 b)laminar BL inside RANS & stability code  BL mode 2 2d two-element configuration: grid: Airbus Results Test Cases & Computational Results

24 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 24 Transition iteration convergence history: BL mode 1 Results pre-prediction phase  1,000 cycles every 20 cycles prediction phase  starts at cycle = 1,000 every 500 cycles fast convergence

25 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 25 c p -field and transition points: BL mode 1 Results -all transition points up- stream of experimental values -no separation in final RANS solution -good approxi- mation of the measured transition points -further im- provement possible using crite- rion for tran- sition in lami- nar separa- tion bubbles

26 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 26 Transition iteration convergence history: BL mode 2, run a Results pre-prediction phase  1,000 cycles every 20 cycles prediction phase  starts at cycle = 1,000 every 1,000 cycles stops at cycle = 10,000 no convergence 1 st numerical instability on flap  induced by transition iteration 2 nd numerical instability on main  induced by RANS procedure

27 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 27 Transition iteration convergence history: BL mode 2, run b Results pre-prediction phase  1,000 cycles every 20 cycles prediction phase  starts at cycle = 1,000 every 500 cycles limited convergence 1 st numerical instability on flap  remains 2 nd numerical instability on main  damped by the procedure

28 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 28 c p -field and transition points: BL mode 2 Results -all transition points down- stream of experimental values -two separa- tions in final RANS solu- tion -flap separa- tion oscilla- tion remains -improved transition lo- cations using calibrated N factor -individual, au- tomatic shut- down of tran- sition module necessary

29 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 29 M = 0.2, Re = 2.3x10 6,  = – 4°, i HTP = 4° grid: 12 mio. points 32 cells in prismatic layers at HTP: 48 cells in prismatic layers SAE N TS = N CF = 7.0 (arbitrary setting) transition prediction on HTP only, upper and lower sides different mode combinations: a)laminar BL code& stability code & line-in flight cuts  BL mode 1 b)laminar BL inside RANS & stability code & inviscid streamlines  BL mode 2 parallel computation: either 32, 48, or 64 processes 2.2 GHz Opteron Linux cluster with 328 CPUs 3D generic aircraft configuration: Results geometry: Airbus, grid: TU Braunschweig

30 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 30 Results c f -distribution wing sections ( (thick white) skin friction lines (thin black) BL mode 2 BL mode 1

31 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 31 BL mode 2 BL mode 1 Results c p -distribution transition lines ( (thick red with symbols) skin friction lines (thin black)

32 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 32 Results convergence of transition lines calls at cycles: 500, 1000, 1500, 2000 out of 2500 pre-pre- diction un- til cycle: 500 every 20 cycles

33 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 33 Results convergence history of the coupled RANS computations:

34 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 34 Conclusion RANS computations with integrated transition prediction were carried out without intervention of the user. The transition tools work fast and reliable. Complex cases (e.g. transport aircraft) can be handled; experience up to now limited to one component of the aircraft. Use of lam. BL code leads to fast convergence of the transition prediction iteration; not always applicable, because transition may be located significantly downstream of lam. separation. Use of internally computed lam. BL data can lead to numerical instabilities when laminar separations are treated  interaction between different separations can occur  interaction of separation points and transition points: oscillation of separation can lead to oscillation of transition  automatic shut down of transition iteration individually for each wing section or component of the configuration necessary Conclusion and Outlook

35 Andreas Krumbein > 27 June 2007 25th AIAA Applied Aerodynamics Conference, Miami, Florida, Slide 35 In the nearest future: Much, much more test cases generic aircraft case: -  variation - different N factors - transition on all wings of the aircraft - inclusion of fuselage transonic cases physical validation, e.g. F4, F6 (AIAA drag prediction workshop) complex high lift configurations, e.g. from European EUROLIFT projects Setup of Best Practice guidelines Conclusion

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