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Data Assimilation Method for
EFD/CFD Integration
2014/11/20 1
Takumi Ambo, Chen Fang
Department of Aerospace Engineering / Institute of Fluid Science
Tohoku University
Boeing Higher Education Program Presentation
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2014/11/20 2
Background -Aerodynamics of low Re number condition-
Appearance of Small airplanes
Unmanned air vehicle (UAV)
Micro air vehicle (MAV)
Three-dimensionality Generation of wingtip vortex
Flight in Low Re conditions (Re = 104~105)
Aerodynamic characteristics
• Different from High Re number condition
• Nonlinearity
Flow field around wing
• Separation or transition of boundary layer
• Formation of separation bubble
It is necessary to investigate aerodynamic characteristics
on the three-dimensional wing in low Re condition.
Three-dimensional flow field
Schematic diagram of separation bubble
(Muller)
Lift coefficient of NACA0012-34 airfoil
(Anyoji et al,2010)
-0.4
-0.2
0
0.2
0.4
0.6
0.8
-5 0 5 10 15
Re=1.1x104, M=0.21
Cl
[deg]
Unmanned Air Vehicles
(http://en.wikipedia.org/wiki/Unmanned_aerial_vehicle)
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Background -EFD & CFD-
2014/11/20 3
Experimental Fluid Dynamics
(EFD)
Computational Fluid Dynamics
(CFD)
Advantage Advantage
Credible data
(Real flow)
Low cost
Big information content
Disadvantage
Disadvantage High cost
Long experimental time
Limited information
Difference from the real flight
(Wall & Support interference)
Computational accuracy relies
on the scheme and mesh
Complement
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2014/11/20 4
CFD/EFD
(Data Assimilation)
CFD
(Forecast)
EFD
(Observation)
Data Information
Quality Control
Validation
Forecast error
First Estimated Value
Model Improvement
Background -Data Assimilation-
• Data assimilation is an analysis technique in which the observed
information is accumulated into the model state by taking advantage of
consistency constraints with laws of time evolution and physical properties.
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Past Studies
Data assimilation
• Computational Study of Flow around a Delta Wing for Measurement-
Integrated Simulation with Dynamic Wind Tunnel Testing (Shuta Ito, 2013)
2014/11/20 5 Boeing Higher Education Program Presentation
Objective
2014/11/20 6
Make the numerical simulation become high-
precision using Data assimilation method to
understand the aerodynamic phenomenon
Contents
EFD
Calculating Lift coefficient and surface streamline
Force measurement
Flow visualization
CFD
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EXPERIMENTAL FLUID
DYNAMICS (EFD)
2014/11/20 Boeing Higher Education Program Presentation 7
Experimental Equipment
2014/11/20 8
Wind-tunnel
Test model
Low Turbulence Wind Tunnel (Tohoku Univ.)
- Type : closed circuit
- Test section : open type and octagon
- Test section size : cross distance of 0.8 m
- Turbulence intensity : 0.02 %
Wing
- Airfoil : NACA0012
- Chord length : 75 mm
- Span length : 400 mm
- Material :Wood(MDF)
14
0 m
m
400 mm
75
mm
φ 30
Body
- Diameter : 30 mm
- Material : Aluminum
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400 mm
φ30
75 m
m
NACA0012 Airfoil
2014/11/20 9
Measurement method -Force measurement-
Sting six-component balance
(NISSHO-ELECTRIC-WORKS, LMC-61112)
Rated load
・Fx-120 N
・Fy-250 N
・Fz-250 N
Sting six-component balance
LFMM zyc 4/
Calculating Pitching-moment
・Mx-4 N・m
・My-10 N・m
・Mz-10 N・m
1/4 chord length Moment center
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Global Luminescent Oil-Film Skin-Friction
Meter (GLOF method)
• Oil doped with luminescent molecules is put on
the test model.
• Skin friction can be measured to capture time-
changing of emission intensity.
Systems
• Fast camera : Lends and optical filter are set
forward of camera
• Light source:UV-LED units
Luminescent oil film
• Oil:Silicone oil
• Fluorescent dye:Perylene
2014/11/20 10
Measurement method -Visualization-
Fast camera
UV-LED
Model
Skin friction measurement
Global Luminescent Oil Film [GLOF]
Measurement system
・ Fast camera : Lends and optical filter are set forward of camera
・ Light source:UV-LED units
Luminescent oil film
・ Oil:Silicone oil
・ Fluorescent dye:Perylene
・ Oil doped with luminescent molecules is put on the test model.
・ Skin friction can be measured to capture time-changing of emission intensity.
Luminescent oil film on the model -1 -0.5 0 0.5 1
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
y/cx/c
Line of frictional stress
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COMPUTATIONAL FLUID
DYNAMICS (CFD)
2014/11/20 Boeing Higher Education Program Presentation 11
Computation
2014/11/20 12 Boeing Higher Education Program Presentation
𝐷𝜌𝑘
𝐷𝑡= min 𝑃,
𝑅𝑒∞𝑀∞20𝛽∗𝜌𝜔𝑘 −
𝑅𝑒∞𝑀∞𝛽∗𝜌𝜔𝑘 +
𝑀∞𝑅𝑒∞
𝜕
𝜕𝑥𝑗(𝜇 + 𝜎𝑘𝜇𝑡)
𝜕𝑘
𝜕𝑥𝑗 𝛾 ∗
Realization of the laminar flow - turbulence transition calculation
: Turbulence energy equation of Menter SST model
Intermittency factor distribution
(Laminar flow cell γ = 0 , Turbulent flow cell γ = 1)
FaSTAR : Developed by JAXA
Aerodynamic coefficients
Surface streamline
Number of :200万点
Flow
Laminar
Turbulent
Computation
2014/11/20 Boeing Higher Education Program Presentation 13
Flow
*Initial condition : It is decided based on separation position of experimental results.
Assimilation method:Ensemble Kalman Filter (EnKF)
Initial condition Parameter Convergent calculation Filtering Calculation end
The number of the
ensemble :10
Experimental
value
Observation update
Laminar
Turbulent
Control point
Computation
2014/11/20 Boeing Higher Education Program Presentation 14
𝑎𝑦
𝑎𝑥
𝑏𝑦
𝑏𝑥
Difference of observation and model :
𝐻 𝑥 − 𝑦 =𝑎𝑦
𝑎𝑥−𝑏𝑦
𝑏𝑥
Objective function of Kalman filter
(minimization of 𝐽):
𝐽 = 1
2(𝑎𝑦
𝑎𝑥−𝑏𝑦
𝑏𝑥)2
𝑆𝑢𝑟𝑓𝑎𝑐𝑒𝑚𝑒𝑠ℎ 𝑝𝑜𝑖𝑛𝑡
Same position
Computational grid Line of frictional stress
(Experiment)
Test conditions
2014/11/20 15 Boeing Higher Education Program Presentation
Wind-tunnel Low turbulence wind-tunnel
Free-stream velocity [m/s] 30
Angle of Attack, α [deg] -10 ~ 30 [deg]
Measurement Aerodynamic forces, Frictional stress line
Experimental conditions
Free-stream velocity [m/s] 30
Angle of Attack, α [deg] 0 ~ 15
Re 1.5 × 105
Turbulence model Menter SST
Analysis method Steady
Number of grid 2× 106
Calculation conditions
RESULTS
2014/11/20 16 Boeing Higher Education Program Presentation
Results -Lift coefficient-
Lift force
2014/11/20 17
-0.4
-0.2
0
0.2
0.4
0.6
0.8
-5 0 5 10 15 20
Re=2.5x104
Re=5.0x104
Re=1.5x105
CL
Angle of Attack [deg]
-0.4
-0.3
-0.2
-0.1
0
0.1
0.2
0.3
0.4
-4 -2 0 2 4
Re=2.5x104
Re=5.0x104
Re=1.5x105
CL
Angle of Attack [deg]
低Re数領域においては,揚力特性はRe数に大きく依存する.
Re数の減少に伴って揚力傾斜の迎角に対する非線形性が強くなる.
Re=5.0x104以下では,低迎角域で特異な非線形領域が現れる.
Re数の減少に伴い低迎角域における非線形領域は拡大する.
The characteristics of lift force is different from high Re number condition.
Stall angle and maximum lift coefficient are lower.
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-0.4
-0.2
0
0.2
0.4
0.6
0.8
-5 0 5 10 15 20
CL
Angle of Attack [deg]Theory of wing sections (1959)
Re = 1.5 x105
Results - Frictional stress line -
2014/11/20 18
2y/b
x/C
0 0.5
10.
5
1
0
2y/b
x/C
0 0.5
10.
5
1
2y/b
x/C
0 0.5
10.
5
2y/b
x/C
0 0.5
10.
5
1
0
2y/b
x/C
0 0.5
10.
5
1
0
2y/b
x/C
0 0.5
10.
5
1
2y/b
x/C
0 0.5
10.
5
2y/b
x/C
0 0.5
10.
5
1
0
2y/b
x/C
0 0.5
10.
5
1
0
2y/b
x/C
0 0.5
10.
5
1
2y/b
x/C
0 0.5
10.
5
2y/b
x/C
0 0.5
10.
5
1
0
α = -1.5 deg α = -0.5 deg α = 0.5 deg α = 4 deg
α = 8 deg α= 10 deg α = 12 deg
Laminar separation is occurred near trailing edge.
Separation bubble appears after α=-0.5 deg.
Separation bubble shift forward along with
increase of AoA.
Leading edge separation bubble is formed in α=8
deg.
Flow separate from trailing edge in α=10 deg.
Most of flow field is dominated by reverse flow
is α=12 deg.
α = 5 deg
Separation line Reattachment line
Separation
bubble
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Root
Wing tip
Flow
Results -Calculated Lift coefficient-
2014/11/20 19 Boeing Higher Education Program Presentation
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
0 2 4 6 8 10 12 14 16 18
Lif
t co
effi
cien
t, C
l
Angle of Attack, α [deg]
Experiment
SST
Laminar
-0.1
-0.2
-0.3
cp5
Under α= 8 deg :Experimental value ≈ Calculated value.
After α = 8 deg There’re difference between EFD and CFD results.
High AoA Separation bubble in leading edge Convergence is difficult.
Shifting boundary of laminar and turbulent Cl changes.
Results - Calculated Surface streamline, α = 8 deg -
2014/11/20 20 Boeing Higher Education Program Presentation
Experimental frictional stress line
Without transition
0
-0.5
-1
Flow
Transition line locates x/c = 0.1 Transition line locates x/c = 0.2
Transition line locates x/c = 0.3 Transition line defined with 5 control points
To control boundary layer transition points using data assimilation method is
useful as a means for approximating CFD results with EFD results
Summary
• In EFD, force measurement and flow visualization were conducted.
• In CFD, location of transition line influences lift coefficient and
surface streamline.
2014/11/20 21 Boeing Higher Education Program Presentation
Future Works
• Conducting calculation of controlling boundary layer transition points
using data assimilation method.
• Apply this method to other unsteady flow conditions like dynamic wind-
tunnel testing.
Make the numerical simulation become high-precision using Data
assimilation method to understand the aerodynamic phenomenon Experiment and Calculation using same model
were conducted and each results were compared.
2014/11/20 22
Thank you for your attention
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