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Aeroacoustic Optimization of an Axial Fan with Variable Blade Loading Michae ael l Stadler er Michae ael l B. Schmitz Ninsight ebm-papst St. Georgen Graz, Austria St. Georgen, Germany Wolfg fgan ang Laufer er Peter Ragg ebm-papst


  1. Aeroacoustic Optimization of an Axial Fan with Variable Blade Loading Michae ael l Stadler er Michae ael l B. Schmitz Ninsight ebm-papst St. Georgen Graz, Austria St. Georgen, Germany Wolfg fgan ang Laufer er Peter Ragg ebm-papst St. Georgen ebm-papst St. Georgen St. Georgen, Germany St. Georgen, Germany ninsight

  2. Objectives minimize selected bands of the acoustic spectrum • maximize aerodynamic efficiency •

  3. Objectives minimize selected bands of the acoustic spectrum • maximize aerodynamic efficiency • hub 𝑠𝑑 𝑣 shroud 𝑠𝑑 𝑣 This is performed for a fan with varying blade geometry (i.e. each blade is loaded differently).

  4. Traditional development cycle for small axial fans 1. Design the blade geometry 2. Assess aerodynamic performance via CFD 3. Assess aeroacoustic performance via physical prototypes

  5. Traditional development cycle for small axial fans 1. Design the blade geometry 2. Assess aerodynamic performance via CFD 3. Assess aeroacoustic performance via physical prototypes Shortco Sh tcoming mings: s: Spurious noise of physical prototypes • imperfect rotor dynamics • eccentricity of the fan • Vibration of the bearing system • Noise due to secondary flow through the cooling channels • Low geometrical resolution of rapid prototyping •

  6. Traditional development cycle for small axial fans 1. Design the blade geometry 2. Assess aerodynamic performance via CFD 3. Assess aeroacoustic performance via physical prototypes Shortco Sh tcoming mings: s: Spurious noise of physical prototypes • imperfect rotor dynamics • eccentricity of the fan • Vibration of the bearing system • Noise due to secondary flow through the cooling channels • Low geometrical resolution of rapid prototyping • T o avoid this tedious optimization procedure augmentation of design process with aeroacoustic simulation

  7. Outline 1 Variable Blade Loading 2 Winglet 3 4 Turbulator Numerical Model 5 Experimental Setup 6 Results

  8. Outline 1 Variable Blade Loading 2 Winglet 3 4 Turbulator Numerical Model 5 Experimental Setup 6 Results

  9. Variable Blade Loading Blade parameterization by averaged swirl at trailing edge for hub and shroud: 2𝜌 𝑠 ⋅ 𝑑 𝑣 = 𝑂 𝑂 2𝜌 𝑠 ⋅ 𝑑 𝑣 𝑒𝜄 0 𝑠𝑑 𝑣 x

  10. Variable Blade Loading Blade parameterization by averaged swirl at From this, the blade loading may be obtained: trailing edge for hub and shroud: 2𝜌 𝑠 ⋅ 𝑑 𝑣 = 𝑂 ∆𝑞 = 2𝜌 𝜖(𝑠 ⋅ 𝑑 𝑣 ) 𝑂 𝑂 𝜍𝑥 𝑛𝑐𝑚 2𝜌 𝑠 ⋅ 𝑑 𝑣 𝑒𝜄 𝜖𝑛 0 𝑠𝑑 𝑣 x

  11. Variable Blade Loading PARAMETERS FOR EVOLUTIONARY OPTIMIZATION 𝑠𝑑 𝑣 Averaged swirl at trailing edge for hub and shroud hub 𝑠𝑑 𝑣 shroud 𝑠𝑑 𝑣

  12. Variable Blade Loading PARAMETERS FOR EVOLUTIONARY OPTIMIZATION 𝑠𝑑 𝑣 Averaged swirl at trailing edge for hub and shroud hub 𝑠𝑑 𝑣 shroud 𝑠𝑑 𝑣

  13. Variable Blade Loading PARAMETERS FOR EVOLUTIONARY OPTIMIZATION 𝑠𝑑 𝑣 Averaged swirl at trailing edge for hub and shroud hub 𝑠𝑑 𝑣 shroud 𝑠𝑑 𝑣 𝑠𝑑 𝑣 is specified independently for 7 individual blades at hub and shroud 14 parameters

  14. Outline 1 Variable Blade Loading 2 Winglet 3 4 Turbulator Numerical Model 5 Experimental Setup 6 Results

  15. Winglet Parameterization PURPOSE OF THE WINGLET: control the tip vortex • Vortex may collide with the adjacent blade → lead to vibration and associated noise production • Vortex can restrict the flow → decrease the aerodynamic performance

  16. Winglet Parameterization Cut the blade with a cylinder of diameter 0.8 D → cross section l 1.

  17. Winglet Parameterization Cut the blade with a cylinder of diameter 0.8 D → cross section l 1.

  18. Winglet Parameterization Cut the blade with a cylinder of diameter 0.8 D → cross section l 1. Project l orthogonal to cylindrical surface of diameter D → cross section m 2.

  19. Winglet Parameterization Cut the blade with a cylinder of diameter 0.8 D → cross section l 1. Project l orthogonal to cylindrical surface of diameter D → cross section m 2. 3. F 1 (q) : Rotation of m around x → m 1

  20. Winglet Parameterization Cut the blade with a cylinder of diameter 0.8 D → cross section l 1. Project l orthogonal to cylindrical surface of diameter D → cross section m 2. 3. F 1 (q) : Rotation of m around x → m 1 4. F 2 (z) : Rotation of m 1 around c → m 2

  21. Winglet Parameterization Cut the blade with a cylinder of diameter 0.8 D → cross section l 1. Project l orthogonal to cylindrical surface of diameter D → cross section m 2. 3. F 1 (q) : Rotation of m around x → m 1 4. F 2 (z) : Rotation of m 1 around c → m 2 5. F 3 (s) : Translation of m 2 along c → m 3

  22. Winglet Parameterization Closure of winglet surface by multisection extrusion between { m,l } → winglet surface k Leading edge Blade bends towards the suction side Trailing edge Blade bends towards the pressure side

  23. Winglet Parameterization Closure of winglet surface by multisection extrusion between { m,l } → winglet surface k Leading edge Blade bends towards the suction side „Conic Winglet Design“ Radius of curvature varies Trailing edge along the winglet spine Blade bends towards the pressure side

  24. Outline 1 Variable Blade Loading 2 Winglet 3 4 Turbulator Numerical Model 5 Experimental Setup 6 Results

  25. Turbulator Parameterization PURPOSE OF THE TURBULATOR: avoid flow separation along blade Adverse effects of flow separation in axial fans: Increased generation of noise • Reduced cross sectional area of the flow channel → degradation of performance •

  26. Turbulator Parameterization PURPOSE OF THE TURBULATOR: avoid flow separation along blade Adverse effects of flow separation in axial fans: Increased generation of noise • Reduced cross sectional area of the flow channel → degradation of performance • General usage of turbulators: Turn laminar flow into turbulent flow (near the leading edge) • Increase the energy of an already turbulent boundary layer → move the point of flow • separation further downstream (e.g. ailerons of commercial airliners)

  27. Turbulator Parameterization DEFINITION OF THE TURBULATOR GEOMETRY Turbulator spine = parallel curve to the line of flow separation (offset g ) Turbulator cross section = simple step (height t ) t g

  28. Turbulator Parameterization DETERMINATION OF THE LINE OF FLOW SEPARATION either by integral convolution of the velocity field, or • by showing the streamlines for the elements adjacent to the blade •

  29. Turbulator Parameterization TURBULATOR AND RAPID PROTOTYPING Machine: EOS 390 (selective laser sintering of polyamide) For the turbulator to work properly, sharp edges are required Fine details of turbulator not sufficiently resolved → augmentation of optimization process with numerical tools necessary! Note: The final product is created by injection die molding (which can Rapid prototyping specimen easily represent sharp edges).

  30. Outline 1 Variable Blade Loading 2 Winglet 3 4 Turbulator Numerical Model 5 Experimental Setup 6 Results

  31. Numerical Model Aeroacoustic analysis Aerodynamic analysis STAR-CCM+ 8.02 STAR-CCM+ 8.02 LES solver RANS solver WALE subgrid scale k- e - turbulence model Discretization of the complete model All y+ wall model Discretization of 1/7th of the model (rotational symmetry)

  32. Numerical Model Evolutionary Optimization • Parametric geometry generation in the 3D-Modeler of STAR-CCM+ • Restore an identical operating point throughout the optimization (change rpm accordingly) • Objective function evaluation • Differential Evolution via Multi-Objective Genetic Algorithm NSGA-II (Non Dominated Sorting GA) • Assisted by a metamodel to reduce the number of objective function evaluations • Pareto front shows the best possible compromise between noise and efficiency over the selected design space Objective function evaluation Efficiency Restore operating Discretization point Noise Parametric NSGA-II Metamodel Geometry Generator

  33. Numerical Model Evolutionary Optimization • Parametric geometry generation in the 3D-Modeler of Star-CCM+ STAR-CCM+ + Plugin in • Restore an identical operating point throughout the optimization (change rpm accordingly) • Objective function evaluation • Differential Evolution via Multi-Objective Genetic Algorithm NSGA-II (Non Dominated Sorting GA) • Assisted by a metamodel to reduce the number of objective function evaluations • Pareto front shows the best possible compromise between noise and efficiency over the selected design space Efficiency Restore operating Discretization point Noise Parametric NSGA-II Metamodel Geometry Generator

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