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The Influence of Turbulence Model on Wake Structure of TSTs when used with a Coupled BEM-CFD Model Ian Masters, R. Malki, Alison Williams & Nick Croft Marine Energy Research Group Swansea University

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Page 1: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

The Influence of Turbulence Model on Wake Structure of TSTs when

used with a Coupled BEM-CFD Model

Ian Masters, R. Malki, Alison Williams & Nick Croft

Marine Energy Research GroupSwansea University

Page 2: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Modelling Approach

Source: A. Mason-Jones , PhD thesis Cardiff University (2010)

Moving Mesh Approach Time-averaged Approach

Page 3: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Array Modelling

Page 4: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Time-Averaged Influence of Blades

Page 5: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Discretisation of Turbine Blades

Page 6: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Discretisation of Turbine Blades (2)

Page 7: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Impact of Blades on the Flow

Page 8: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Impact of Blades on the Flow (2)

Page 9: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Calculating Resultant Forces

Page 10: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Resolving Forces

Page 11: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Calculating Source Terms (BEMT)

Page 12: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Substituting Source Terms (BEM-CFD)

Page 13: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Substituting Source Terms (BEM-CFD)

Page 14: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Model Domain

0.5m

0.25m

1.4m

0.5m

1.54m

0.84m

0.17m

0.84m

0.17m

Page 15: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Rotor Modelling

Page 16: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Edge Parameters

Page 17: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Edge Characterisation

Page 18: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

95% Wake Edges

P∞

PWAKE

P95%

P∞

Page 19: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

k-epsilon• Eddy viscosity from single length scale• Turbulent diffusion occurs only at specified scaleRNG k-epsilon• Account for different scales of motionk-omega• Viscous sub-layer flows• Adverse pressure gradients and separating flows

Turbulence Models

Page 20: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Shear Stress Transport (SST)• k-ω near boundary• k-ε in free-stream• Adverse pressure gradients & separating flowsReynolds Stress Model (RSM)• Reynolds Stresses directly computed• Directional effects of Reynolds stress fields• More suitable for anisotropic turbulence

Turbulence Models

Page 21: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Velocity

Page 22: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Velocity

Page 23: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Velocity

Page 24: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Turbulence Intensity

Page 25: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Turbulence Intensity

Page 26: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Turbulence Intensity

Page 27: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Turbulent Viscosity

Page 28: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Lateral Shear

Page 29: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Velocity ProfilesTSR = 4.0

Page 30: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Velocity ProfilesTSR = 4.0 & 6.0

Page 31: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

TI ProfilesTSR = 4.0

Page 32: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

TI ProfilesTSR = 4.0 & 6.0

Page 33: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Diameter 95% Velocity

TSR = 4.0

Page 34: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Diameter 95% Velocity

TSR = 4.0 & 6.0

Page 35: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Diameter 95% TI

TSR = 4.0

Page 36: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Diameter 95% TI

TSR = 4.0 & 6.0

Page 37: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Diameter 95% dUdz TSR = 4.0

Page 38: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Wake Diameter 95% dUdz

TSR = 4.0 & 6.0

Page 39: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

• Turbulence Models affect Hydrodynamics• Lack of Measured Data for Validation• Possibly better represent turbulence

Conclusions

Page 40: Source: A. Mason-Jones, PhD thesis Cardiff University (2010) Moving Mesh ApproachTime-averaged Approach

Rotor Source Terms