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EUROGEN 2011Mainstream Session 7: Aerospace
1
D i P f I ti ti f M difi d PARSECD i P f I ti ti f M difi d PARSECDesign Performance Investigation of Modified PARSEC Airfoil Representation Using Genetic Algorithm
Design Performance Investigation of Modified PARSEC Airfoil Representation Using Genetic Algorithm
•Tomoyoshi YotsuyaTokyo Metropolitan University
•Masahiro KanazakiTokyo Metropolitan University
•Kisa MatsushimaKisa MatsushimaToyama University
ContentsContents2
1. Background2 Objectives2. Objectives3. Airfoil Representation Methods4. Optimization Method Multi-objective genetic algorithm (MOGA)j g g ( ) Data mining method
5 Computational fluid dynamics5. Computational fluid dynamics6. Formulations7. Results8. Conclusions8. Conclusions
3
BackgroundBackgroundDevelopment of airfoils High fidelity Computational Fluid High fidelity Computational Fluid
Dynamics (CFD) have been applied to real world design problems with
i f il/ i b d i d i
to real-world design problems with high-performance computing.
Airfoil/wing can be designed using evolutionally algorithm with CFD ffi i l f i f
Blended wing body aircraft
efficiently for new concept aircraft.
Efficient geometry representation is requiredSupersonic aircraft Mars exploration aircraft
for computer aided design.
Effi i i f il i
4
BackgroundBackgroundEfficient airfoil representation
U f d l fPARSEC(PARametric SECtion) method*
Upper surface and lower surface are separately defined.Parameterization geometrical character based on knowledge of transonic flowEasy to understand design informationA few geometrical parameters around the leading-edge
modification Modified PARSEC method**
Thickness distribution and camber are designedcamber are designed.This definition is in theory of wing section
*Sobieczky, H., “Parametric Airfoils and Wings,” Notes on Numerical Fluid Mechanics, pp. 71-88, Vieweg 1998.** Matsuzawa, T., et al, Application of PARSEC Geometry Representation to High-Fidelity Aircraft Design byCFD, K. Matsushima, CD proceedings of 5th WCCM/ ECCOMAS2008, Venice, CAS1.8-4 (MS106), 2008.
ObjectivesObjectives5
• Investigation of design performance by Modified PARSEC representationModified PARSEC representation.– Comparison of airfoil design performance among
i i l d d difi ioriginal and two proposed modifications
For this investigation, two design problem are solved.g , g p1. Conventional transonic airfoil design problem2. Airfoil design problem for low Reynolds number
Airfoil Representation MethodsAirfoil Representation Methods6
Original PARSEC (PARSEC11) method
It d i t i i f il ith f d i i blAd tis defined upper and lower surface.
Because the leading-edge radius centre is supposed on the x-axis, it h diffi lt t i th d i f d
It can design transonic airfoil with a few design variables.
Disadvantage
Advantage
it has difficulty to improve the aerodynamic performance around the leading-edge for an airfoil which has large camber.
Disadvantage
→ Only rle decides the leading edge geometry.
upper surface2
126
n
Number of design variables is 11.
y le g g g y
2
1|
xazn
nlowup
lower surface
Airfoil Representation MethodsAirfoil Representation Methods7
Modified PARSEC method 1is defined by thickness distribution and camberis defined by thickness distribution and camber .
The leading edge radius centre is always on the camber. The thickness distribution is same as symmetrical airfoil by
PARSEC method. The camber is defined by a quintic equation. N b f d i i bl i 11
Thickness distribution Camber
5nxbz126 n
Number of design variables is 11.
1n
nc xbz
+
212
1
n
xazn
nt
+
Airfoil Representation MethodsAirfoil Representation Methods8
Modified PARSEC method 2is added design parameters for leading edge camber.
In camber definition, the square root term is added to improve design performance around the leading edge.
g p g g
By adding the root term, the design performance of the leading-edge is improved.
N b f d i i bl i 12 Number of design variables is 12.
5Camber
5
10
n
nnc xbxbz
Optimization MethodOptimization Method9
Adaptive Range Divided Range Multi-Objective Genetic Algorithm (ARDRMOGA)g ( )Adaptive Range scheme*
Advantage: global exploration design spaceDivided Range scheme**
Advantage: maintain high diversity
The flow chart of ARDRMOGA
*Sasaki, D., et al, “Efficient search for trade-offs by adaptive range multi-objective genetic algorithms,” Journal of Aerospace Computing, Information and Communication, pp. 44-64, 2005.**Hiroyasu , T., et al, The new model of parallel genetic algorithm in multi-objective optimization problems (divided range multi-objective genetic algorithm), IEEE Proceedings of the Congress on Evolutionary Computation 2000, Vol. 1, pp. 333-340, 2000.
Optimization MethodOptimization Method10
Adaptive range (AR) Search region is changed according to standard deviation. The solution space can be explored without an oversight of
optimum solutions. The new decision space is determined based on the The new decision space is determined based on the
statistics of selected better solutions. The new population is generated in the new decision space.The new population is generated in the new decision space.
Optimization MethodOptimization Method11
Divided range (DR) The population is divided and sorted by design space. DR scheme can prevent the crossover between the
scattered parents. DR scheme maintain high diversity DR scheme maintain high diversity. Every MDR generation, sorted function is switched.
Every MDRgenerationgeneration
Data Mining MethodData Mining Method12
P ll l C di Pl (PCP)Parallel Coordinate Plot (PCP) One of statistical visualization techniques from high-
dimensional data into two dimensional datadimensional data into two dimensional data. Design variables and objective functions are set parallel in the
normalized axis. PCP shows global trends of design variables and objective
functions. 0 81.0
0 20.4 0.6 0.8
0.0 0.2
dv1
dv2
dv3
dv4
dv5
dv6
dv7
dv8
dv9
v10
v11
v12
v13
v14
L/D
ΔP ing
Upper bound of ith design variables and objective functions
Lower bound of ith design variables)min(-)( ii dvdvxP
Normalization
d d d d d d d d d dv dv dv dv dv L Δ
Wwi
Lower bound of ith design variables and objective functions )min(-)max( ii
i dvdvP
FormulationsFormulations13
Mach Number : 0.8 (240 m/s)Reynolds Number : 1 0×107
Case1 : Conventional transonic airfoil design
Reynolds Number : 1.0×107
Altitude : 1.0×104 [km]Case2 : Airfoil design for low Reynolds numberCase2 : Airfoil design for low Reynolds number
(to use Mars exploration aircraft project(ISAS/JAXA))Mach Number : 0.52 (120 m/s)
ld b 3 0 104Reynolds Number: 3.0×104
Altitude : Ground level
Objective FunctionsMaximize Airfoil thickness (t)Minimize Drag coefficient (Cd)
Subject to lift coefficient (Cl) = target Cl- Case1 : Cl =0 0, 0 4Case1 : Cl 0.0, 0.4- Case2 : Cl =0.6, 0.8
14
CFD MethodCFD Method
Two dimensional Navier-Stokes flow solverTwo dimensional Navier Stokes flow solver0
ndsFQdVt
Time integration : LU-SGS implicit methodFlux evaluation : Third-order-accuracy
i d diff ti l h Airfoil grid viewupwind differential schemewith MUSCL method
Turbulent model : Baldwin-Lomax model
Airfoil grid view
Turbulent model : Baldwin Lomax model
Computational grid
Grid : C-H type structured gridGrid size 23,000 p g
Design VariablesDesign Variables15
Design space for case1
PARSEC methodCl=0.0 Cl=0.4
Modified method 1Cl=0.0 Cl=0.4
Modified method2Cl=0.0 Cl=0.4
lower upper lower upperrle 0.005 0.040 0.004 0.040αte -8.0 -3.0 -8.0 0.0
lower upper lower upperrle 0.005 0.040 0.004 0.040xt 0.4 0.5 0.4 0.5
lower upper lower upperrle 0.005 0.040 0.004 0.040xt 0.4 0.5 0.4 0.5
xup 0.4 0.5 0.3 0.5zup 0.04 0.12 0.04 0.12zxxup -1.1 -0.4 -1.0 -0.4
zt 0.04 0.10 0.02 0.08zxxt -1.0 -0.4 -1.0 -0.1βte 4.4 6.4 4.4 6.4
zt 0.04 0.10 0.02 0.08zxxt -1.0 -0.4 -1.0 -0.1βte 4.4 6.4 4.4 6.4
xlo 0.35 0.50 0.35 0.50zlo -0.08 -0.04 -0.05 0.02zxxlo 0.2 1.0 0.3 1.0β 4 4 6 6 4 0 8 0
xc 0.30 0.50 0.35 0.50zc 0.00 0.04 0.00 0.07zxxc -0.5 0.0 -0.7 0.0
0 01 0 02 0 01 0 02
rc 0.000 0.002 0.000 0.004xc 0.30 0.50 0.35 0.50zc 0.00 0.04 0.00 0.07
0 5 0 0 0 7 0 0βte 4.4 6.6 4.0 8.0zte -0.01 0.02 -0.02 0.02
zte -0.01 0.02 -0.01 0.02αte 3.0 8.0 0.0 8.0
zxxc -0.5 0.0 -0.7 0.0zte -0.01 0.02 -0.01 0.02αte 3.0 8.0 0.0 8.0
Design VariablesDesign Variables16
Design space for case2
PARSEC methodCl=0.6 Cl=0.8
Modified method1Cl=0.6 Cl=0.8
Modified method2Cl=0.6 Cl=0.8
lower upper lower upperrle 0.004 0.040 0.004 0.040αte -8.0 0.0 -8.0 0.0
lower upper lower upperrle 0.004 0.040 0.004 0.040xt 0.4 0.5 0.4 0.5
lower upper lower upperrle 0.004 0.040 0.004 0.040xt 0.4 0.5 0.4 0.5
xup 0.3 0.5 0.3 0.5zup 0.04 0.12 0.04 0.12zxxup -1.0 -0.4 -1.0 -0.4
zt 0.02 0.08 0.02 0.08zxxt -1.0 -0.1 -1.0 -0.1βte 4.4 6.4 4.4 6.4
zt 0.02 0.08 0.02 0.08zxxt -1.0 -0.1 -1.0 -0.1βte 4.4 6.4 4.4 6.4
xlo 0.35 0.5 0.35 0.5zlo -0.05 0.02 -0.05 0.02zxxlo 0.3 1.0 0.3 1.0β 4 0 8 0 4 0 8 0
xc 0.35 0.50 0.35 0.50zc 0.00 0.07 0.00 0.07zxxc -0.7 0.0 -0.7 0.0
0 01 0 02 0 01 0 02
rc 0.000 0.004 0.000 0.004xc 0.35 0.50 0.35 0.50zc 0.00 0.07 0.00 0.07
0 7 0 0 0 7 0 0βte 4.0 8.0 4.0 8.0zte -0.02 0.02 -0.02 0.02
zte -0.01 0.02 -0.01 0.02αte 0.0 8.0 0.0 8.0
zxxc -0.7 0.0 -0.7 0.0zte -0.01 0.02 -0.01 0.02αte 0.0 8.0 0.0 8.0
17
ResultsCase1 : Conventional transonic airfoil design
Case2 : Airfoil design for low Reynolds numberCase2 : Airfoil design for low Reynolds number
Result (case1)Result (case1)18
Optimization resultNon-dominated solutions
Design C =0 0 Design Cl=0 4Design Cl=0.0 Design Cl 0.4
Optimum direction Optimum direction
There are trade-off between objective functions in each case. Modified method could generate good solutions as well as the
original PARSEC method.
Result (case1, Cl=0.4)Result (case1, Cl=0.4)19
Thi k f d 1Design Cl=0.4 Thickness distribution
0.06
Thickness of des1Thickness of des2Thickness of des3
0.00 0 0 0 5 1 0
0.04 C b f d 1Camber
-0.06
0.0 0.5 1.0
0.02
0.04 Camber of des1Camber of des2Camber of des3
Camber
0.000 0 0 5 1 0
Des1D 3
AoA=-0.6°0.0 0.5 1.0
Des1-3 are selected from non-dominated solutions. (t/c are about 0.10 t/c)Des2
Des3
A A 0 3°
AoA=-0.3°
Des1-3 has maximum camber at trailing edge.Des3 has largest camber around leading edge.
AoA=-0.3°
Result (case1, Cl=0.4)Result (case1, Cl=0.4)20
Pressure distributionDes1 (PARSEC method) -1.00
-0.50 0 0 0 5 1 0
Pressure distributionAoA = -0.6°
0.00
0 50
0.0 0.5 1.0
upper surfacelower surface
Des2 (Modified method 1)0.50
-1.00
-0.50 0 0 0 5 1 0
AoA = -0.3°
0.00
0 50
0.0 0.5 1.0
upper surfacelower surface
Des3 (Modified method 2)
0.50
AoA = -0.4°-1.00
-0.50 0 0 0 5 1 0
S h C di ib i i D 3
0.00
0.50
0.0 0.5 1.0
upper surfacelower surface
Smooth Cp distribution in Des3 -Modified2 has possibility to design airfoil which achieves lower wave drag.
Result (case1, Cl=0.4)Result (case1, Cl=0.4)21
0.8 1.0
PARSEC methodDesign informationPCP visualizes 10 individuals which achieve low Cd.
0 20.4 0.6 The trend of αte is same tendency
among three methods.The trend of x and x is different from
achieve low Cd.
0.0 0.2
rle
αte
xup
zup
xup
xlozlo
xxlo βtezte tcd
The trend of xup and xt is different from that obtained by modified method 2.
→Because of rc , xt is smaller to control leading edge in modification 2 x z
zxx zx
1.0 1.0 Modified method 1 Modified method 2
control leading edge in modification 2.
0 40.6 0.8
0 40.6 0.8
0.0 0.2 0.4
0.0 0.2 0.4
rle xt zt
zxxt βte xc zc
zxxc zte
αte tcd rle xt zt
zxxt βte rc xc zc
zxxc zte
αte tcd
22
ResultsCase1 : Conventional transonic airfoil design
Case2 : Airfoil design for low Reynolds numberCase2 : Airfoil design for low Reynolds number
Result (case2)Result (case2)23
Optimization resultNon-dominated solutions
Design C =0 6 Design Cl=0 8Design Cl=0.6 Design Cl 0.8
Optimum direction Optimum direction
Thinner airfoils can be obtained by modified methods. The thinner airfoil cannot be designed by the originalThe thinner airfoil cannot be designed by the original
PARSEC method.
Thickness of des4Result (case2, Cl=0.8)Result (case2, Cl=0.8)
24
D i C 0 80.05
Thickness of des4Thickness of des5Thickness of des6
Design Cl=0.8 Thickness distribution
0.00 0.0 0.5 1.0
Camber of des4
-0.05
Camber
0.05
Camber of des4Camber of des5Camber of des6
D 4
Camber
00.0 0.5 1.0
Des4AoA=4.5°
Des5Des6Des1-3 are selected from non-dominated
solutions. (t/c are about 0.07 t/c)Each airfoil has large camber
AoA=3.5°AoA=2 9° Each airfoil has large camber.
The surface of Des4 is not smooth.AoA=2.9
Result (case2, Cl=0.8)Result (case2, Cl=0.8)25
Pressure distributionDes4 (PARSEC method) -1.50
0 000.0 0.5 1.0
Pressure distributionAoA=4.5°
0.00
1.50 upper surfacelower surfacd
1 50Des5 (Modified method 1)
-1.50
0.00 0.0 0.5 1.0 AoA=3.5°
1.50 upper surfacelower surfacd
-1.50
Des6 (Modified method 2)
.50
0.00 0.0 0.5 1.0
AoA=2.9°
The thickness distributions are smooth in 1.50
upper surfacelower surfacd
Des5 and 6.→Smooth flow on airfoil.
Result (case2, Cl=0.8)Result (case2, Cl=0.8)26
PARSEC th d
0.8 1.0
PARSEC methodDesign informationPCP visualizes 10 individuals which achieve low Cd.
0.20.4 0.6
d
The trend of rle is similar.In PARSEC method, αte is smaller.
→ It cannot represent airfoils with
In modified method 2, the influence of rcis significant.
0.0 0.2
rle
αte
xup
zup
xxup xlozlo
xxlo βtezte tCd
plarge camber.
zx zx
1.0 1.0 Modified method 1 Modified method 2
0 40.6 0.8
0 40.6 0.8
0.0 0.2 0.4
0.0 0.2 0.4
0.0
rle xt zt
zxxt βte xc zx
zxxc zte
αte tCd
0.0rle xt zt
zxxt βte rc xc zc
zxxc zte
αte tCd
ConclusionsConclusions27
Investigation of design performance modified method PARSEC representation by MOGAmethod PARSEC representation by MOGA. Solving two kinds of airfoil design problems by MOGA;
1) transonic airfoil, and 2) low Reynolds number airfoil) , ) y Comparisons of design results among original and modifications
– In conventional transonic airfoil design, modified methods ld d i d f i f il ll th i i lcould design good performance airfoil as well as the original
PARSEC method.• In modification2, the local shock is weaken.
– In airfoil design for low Reynolds number, modified method have the potential to design better airfoils than that of the original methodoriginal method.
• Modified method can be represent smooth surface airfoils with large camber.
• Modified methods design leading edge camber well.
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Thank you for your attentionThank you for your attention