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Atmospheric Flow over Terrain using Hybrid RANSLES

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Title: Atmospheric Flow over Terrain using Hybrid RANSLES


1
  • Atmospheric Flow over Terrain using Hybrid
    RANS/LES
  • European Wind Energy Conference Exhibition 2007
  • A. Bechmann, N.N. Sørensen and J. Johansen
  • Wind Energy Department
  • Risoe National Laboratory
  • Technical University of Denmark
  • andreas.bechmann_at_risoe.dk

2
  • Appetizer
  • Simulation of Wind over Complex Terrain

3
Outline
  • Introduction Terrain flow using CFD
  • New approach Hybrid RANS/LES model
  • Simulation results Askervein Hill
  • Conclusions

4
Introduction Complex terrain?
5
Introduction Why CFD?
  • Structural loads in complex terrain - most
    important issue
  • The critiquel wind happens locally - difficult to
    measure
  • Computational fluid dynamics (CFD) -provides
    supplemant

6
Introduction EllipSys3D code
  • Risø/DTU code, Applications
  • Terrain computation
  • Airfoil computations
  • Rotor computations
  • EllipSys3D code
  • Incompressible Navier-Stokes
  • Finite-volume (non-staggered)
  • Pressure/Velocity formulation
  • Patched multi-block grids
  • Parallellized using MPI for distributed computers

7
Introduction problem formulation
  • RANS-method
  • Provides the mean wind speed and turbulence
    intensity
  • Average amount of modelling
  • Wall-func. easily implemented
  • Computational affordable
  • Complex terrain
  • Wall-functions are needed due to surface
    roughness (buildings, grass, trees etc.)
  • Simple flow models for complex terrain are
    unreliable.
  • The unsteady wind is important when predicting
    wind loads
  • LES-method
  • Provides detailed and transient wind information
  • Minimum of modelling needed
  • Wall-functions are problematic
  • Near-surface flow is computational very expensive

8
Outline
  • Introduction Terrain flow using CFD
  • New approach Hybrid RANS/LES model
  • Simulation results Askervein Hill
  • Conclusions

9
New approach basic equations
  • Stress term replaces viscosity term (high Re)
  • RANS- and LES-equations written in same form
  • different only by how stress term is modelled

10
New approach turbulence model
Similar to Detached-Eddy Simulation Spalart et
al. (1997)
11
New approach turbulent lengthscale
12
New approach turbulent lengthscale
13
Outline
  • Introduction Terrain flow using CFD
  • New approach Hybrid RANS/LES model
  • Simulation results Askervein Hill
  • Conclusions

14
Askervein hill background
  • Askervein hill
  • Hebrides, Scotland. 1982-1983
  • H116m, planform 2x1km
  • Computational grid
  • N288x240x96 (7mill cells)
  • Domain size 8.8x5.5x1.5 km
  • Resolution ?23m, z10.03m

15
Askervein hill precursor
  • Precursor
  • Wind over flat-terrain with homogeneous roughness
  • Simulation is run until statistics are converged
  • Velocity slice are stored at each timestep
  • Successor
  • Wind over terrain with in- homogeneous roughness
  • Variables are read at each timestep
  • At least one flow through time before results are
    sampled

16
Askervein hill flow field
17
Askervein hill speed-up
18
Askervein hill turbulence
19
Outline
  • Introduction Terrain flow using CFD
  • New approach Hybrid RANS/LES model
  • Simulation results Askervein Hill
  • Conclusions

20
Conclusions
21
  • Thank you for listening!
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