Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic...

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SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical study of the tip vortex (Application to Kaplan Turbine) J.Decaix, (HEVS) M. Dreyer, (LMH-EPFL) C. Münch-Alligné, (HEVS) M. Farhat, (LMH-EPFL) 1

Transcript of Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic...

Page 1: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

Experimental and numerical study of the tip vortex (Application to Kaplan Turbine)

J.Decaix, (HEVS) M. Dreyer, (LMH-EPFL) C. Münch-Alligné, (HEVS) M. Farhat, (LMH-EPFL)

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Page 2: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

OVERVIEW OF THE PRESENTATION

1.Hydronet 2 Project 2.Experimental Part 3.Numerical Part 4.Experiment vs Numerical 5.Conclusion

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Page 3: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

Hydronet 2 Project

Multidisciplinary consortium

Simulation of sand erosion

Tip vortex cavitation

Instability of pump-turbine

HydroPower design

Plant monitoring

To improve the Design, Manufacturing and Operation of HydroPower Plants

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Page 4: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

TIP VORTEX CAVITATION (TVC)

Problematic: • Tip vortex cavitation → severe erosion in axial turbines • Origin: vortex roll up in the gap at the tip of the blades • Remedy (anti-cavitation lip): inefficient • Influence of gap width? • Scale up rules? (actual model tests not reliable)

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Page 5: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

TIP VORTEX CAVITATION (TVC)

Goals : Experimental and numerical investigations of TVC for a better understanding of the physical phenomena Case study: Naca0009 hydrofoil with variable gap width

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Page 6: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

EXPERIMENTAL PART

Tools : • Stereo PIV (Particle Image Velocimetry)

Goals : Measure the tip vortex velocity field for various operating conditions:

• Inlet velocity: 5 m/s → 20 m/s • Incidence angle: 3° → 12° • Gap width: 0 mm → 20 mm

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Page 7: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

EXPERIMENTAL PART Stereo PIV setup:

• LMH cavitation tunnel

• Hydrofoil: Naca0009

• Variable gap width

• 200 mJ YAG laser

• Seeding particles: 20 µm hollow glass spheres

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Page 8: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

EXPERIMENTAL PART

PIV working principle:

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Page 9: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

EXPERIMENTAL PART Stereo PIV principle:

Need of a proper optical calibration!

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Page 10: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

EXPERIMENTAL PART Stereo PIV setup:

Combining the left and right velocity field: 3D velocity field

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Page 11: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

EXPERIMENTAL PART Velocity field processing:

• Correction of vortex wandering • Mean velocity and vorticity field calculation

Instantaneous Vortex center

Realignment of velocity field before averaging!

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Page 12: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

NUMERICAL PART

Goals : To perform the numerical simulations of the experimental cases

Tools : • Ansys CFX 14.0 commercial solver • OpenFoam 2.1.0 open source solver

Modelling : Reynolds Average Navier-Stokes computations coupling with standard two-equations turbulence models : k-ε or k-ω SST

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Page 13: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

FIRST COMPUTATIONS Configurations :

• Incidence angle : α = 10° • Inlet velocity : Uinlet = 5.4 m/s or 10.2 m/s Regap ≈ 105

• Gap value : 5 mm, 10 mm and 15 mm

Mesh : 2.9 millions of points with 30 points in the gap

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Page 14: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

COMPARISON BETWEEN SOLVERS Position of the tip vortex measured from the maximum of the Q-criterion

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Configuration: U = 10.2 m/s , α = 10°, gap = 10 mm

Page 15: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

Q-Criterion

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z

y

Definition

Q = 1/2 (||Ω||2 −||S||2)

With: • Ω: Rotation rate tensor • S: Strain rate tensor

Page 16: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

COMPARISON BETWEEN SOLVERS

Vertical position of the tip vortex downstream the Naca

Configuration : • Uinlet = 10.2 m/s • α = 10°

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Page 17: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

COMPARISON BETWEEN SOLVERS

Spanwise position of the tip vortex downstream the Naca

Configuration : • Uinlet = 10.2 m/s • α = 10°

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Page 18: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

COMPARISON BETWEEN COMPUTATIONS AND EXPERIMENT

Comparisons : • Done on a plan located 35 mm downstream the

trailing edge x = 85 mm

• Focus on the velocity and vorticity fields

• Position of the vortex core determined from the axial

vorticity

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Page 19: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

AXIAL VORTICITY

Experiment Computation (OpenFoam)

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Configuration: U = 10.2 m/s , α = 10°, gap = 10 mm

Page 20: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

VORTEX POSITION Configuration: α = 10° ; U = 10.2 m/s ; Gap = 10 mm

Page 21: Experimental and numerical study of the tip vortex …SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes. June 5-6th, 2013, Grenoble, France Experimental and numerical

SHF Conference on Cavitation, Hydraulic Machines. Air in Water Pipes.

June 5-6th, 2013, Grenoble, France

CONCLUSION AND OUTLOOK

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Experimental Part PIV set up with correction of the wandering motion Acquisition of data for several flow configurations Analysis of the velocity and vorticity fields evolution with

tip vortex confinement

Numerical Part Comparison between CFX 14.0 and OpenFoam 2.1.0 for

different flow configurations Comparison between solver results and experimental data

for different flow configurations

FUTURE A deeper investigation of the tip vortex in cavitating and non-cavitating configurations