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Advanced Aerodynamic Analysis of the NASA High-
Lift Trap Wing with a Moving Flap Configuration
Matt Hieatt
• Introduction
• Numerical Methodology
• 1st High Lift Prediction Workshop and Results
• Polar Sweep
• Stowing and Un-Stowing
• Summary
Outline
2
XFlow is a CFD software specifically designed to simulate complex systems
with highly transient flows and the presence of moving parts
These two areas have traditionally proven to be difficult to treat with classic
FEM/FVM schemes
Introduction
3
• Inspired by the kinetic theory of gases
The kinetic theory of gases is a physical theory that explains the macroscopic behavior and properties of gases from a statistical description of the microscopic molecular processes (L. Boltzmann, J.C. Maxwell, s. XIX)
• Solves the Boltzmann equation across an octagonal grid
• The fluid is represented as particle distribution functions (PDFs) of linear momentum and density
Streaming Transport of the PDF’s to surrounding points
Distribution Models the Interaction and scatter of molecules to recalculate the PDF’s
Lattice-Boltzmann Method
Lattice-Boltzmann Method
5
• No meshing required
• Inherently transient and compressible
• Solves Large Eddy Simulation to resolution of the grid
• Dynamically increases resolution to capture turbulence
• Automatically detects geometry and applies
advanced wall model (fixed or moving)
• Introduction
• Numerical Methodology
• 1st High Lift Prediction Workshop Results
• Polar Sweep
• Stowing and Un-Stowing
• Summary
Outline
6
• Trap wing "Config 1" (slat 30, flap 25)
• Mach = 0.2
• Reynolds = 4.3E+6 based on MAC
• Mean aerodynamic chord = 1.0067 m
• AoA: -4, 1, 6, 13, 21, 28, 32, 34 and 37 degrees
1st High Lift Prediction Workshop Results
7
All the computations were run on a single workstation with twoprocessors Intel Xeon E5620 @ 2.4 GHz (8 cores) and 12GB of RAM
The American Institute of Aeronautics and Astronautics (AIAA)is the world'slargest technical society dedicated to the global aerospace profession
The 1st AIAA CFD High Lift Prediction Workshop1 (HiLiftPW-1) took place inJune 2010,provided a reference benchmark for the aeronautical industry, totest commercial CFD software packages.
1st High Lift Prediction Workshop Results
8
Virtual wind tunnel configuration: ( 40 x 15 x 30 ) m
Far field velocity as initial boundary condition
Slip plane on the boundary wall
Periodic Boundaries elsewhere
Model Set up
Lattice Size and Convergence Study
Spatial discretization
Each refinement level solves spatial and temporal scales two times smaller than theprevious level
Resolved scale = h Resolved scale = h/2 Resolved scale = h/4
Resolved scale = h and target scale near walls = h/4
1st High Lift Prediction Workshop Results
Lattice size and Convergence study
12
CaseMach
numberReynolds number
MAC (m)
Simulationtime (s)
Theoricalboundary layer thickness (m)
Farfieldrefinement
(m)
Near wallrefineme
nt (m)
Wake refinemen
t (m)
Numberelement
Cells # onMAC
Cells # in boundary
layer
Cells # onFarfield (x direction)
HL1 0.2 4.30E+06 1.0067 0.3 0.0181 1.28 0.01 0.02 2.89E+06 100.67 1.81 31.25
HL2 0.175 1.50E+07 0.34709 0.1 0.0049 5.12 0.005 - 1.50E+08 69.41 0.97 7.81
HL2 0.175 1.51E+08 0.34709 0.1 0.0031 5.12 0.005 - 1.50E+08 69.41 0.61 7.81
HTP forward 0.2 1.90E+06 0.431 0.5 0.0091 1.28 0.005 0.01 7e6 to 35e6 86.20 1.83 31.25
UAV 0.1 1.50E+06 0.69 0.5 0.0153 1.28 0.01 0.02 5.00E+06 69 1.53 46.87
Recommended values:
Lattice nodes on MAC ≈ 85 lattices
Lattice nodes in boundary layer ≈ 1.5 lattices
Lattice nodes in the Farfield x-direction ≈ 20 lattices
Wake refinement twice wing refinement
Aerospace “Hygiene” Rules
• Introduction
• Numerical Methodology
• 1st High Lift Prediction Workshop Results
• Polar Sweep
• Stowing and Un-Stowing
• Summary
Outline
17
• Introduction
• Numerical Methodology
• 1st High Lift Prediction Workshop Results
• Polar Sweep
• Stowing and Un-Stowing
• Summary
Outline
22
• Results for the 1st HLPWF in good agreement with experimental
data
• XFlow has been proved a reliable tool for traditional and advanced
aerodynamic problems involving presence of moving parts
• Successful polar sweep simulation
• Proof of concept simulation for the stowing and un-stowing
maneuvers shows interesting results
Summary
27