ADJOINT BASED AEROELASTIC SHAPE OPTIMIZATION OF A SLENDER WING MOUNTED ON A LOITERING MUNITION
5th Annual SU2 Conference
1 October 2024
Ongoing MSc Study By:
Emirhan Evin
Supervisor : Prof. Dr. İsmail H. Tuncer
OUTLINE
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Emirhan Evin
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INTRODUCTION
Tube/Air launched munitions face difficulties while opening their wings or control surfaces due to the excessive final deflection and root bending moments. This problem became more important with the increased popularity of loitering munitions.
Altius 700 – An example of Air Launch
Hero 30 – An example of Tube/Ground Launch
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PROBLEM DEFINITON
Conceptual Configuration
The main objective of the study is to optimize the wing geometry of a tube/air launched munition to minimize;
While;
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PROBLEM DEFINITON
Simple thinplate is chosen to model wing structure. Although more complex wing structure models have been tried none of them converged / deformed successfully.
130 mm
60 mm
1070.25 mm
This part has 6mm thickness
This part has 8mm thickness
Clamped boundary condition is assigned to the blue part on the figure. �Wing structure model starting from 11.25% of the chord length. The distance is approximately 22.5mm
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PROBLEM DEFINITON
Placement of the thinplate structure inside the wing
Following structural models were tried but failed.
Thick, hollow shell
Rib – Spar formation
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FLUID DOMAIN PROPERTIES
Farfield :: L=30m, D=20m
Farfield and all sources are in the form of cylinder.�
Fluid domain mesh is unstructred. All the sources are used to cluster mesh close to the body and refine the expansion of the cells to the farfield.
Source1 :: L=16.5m, D=11m
Source2 :: L=9m, D=6m
Source3 :: L=3.6m, D=2.4m
Geometry
5th Conference - 2024
4.5 m
2.5 m
1.8 m
3.6 m
5.0 m
9.0 m
Alignment of the sources can be seen in this figure.
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FLUID DOMAIN PROPERTIES
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FLOW SOLUTION
With the given setup, 4 different fluid meshes are obtained, here the results of the wings only.
Solver : RANS
Turb. Model : SST – V2003m
Mach : 0.1
Alpha : 0°
Beta : 0°
Density : 1.11164 kg/m3
Viscosity : 1.758e-5
Speed of Sound: 336.434 m/s
Temperature : 281.65 K
Pressure : 89874.56 Pa
Re : 4.255e5
First cell height to achieve y+ ~1: 1.0405e-5 m
Required layer amount: 27
Altitude : 1000 m
Conv Criteria : RMS<1e-10
Num. Method : JST
#cells [m] | CFx | CFy | CFz | CMx | CMy | CMz | CMx [W1] | CMx [W2] |
12.66 | 0.024979 | 0.001236 | 0.254923 | -0.00143 | -0.00956 | -8.7E-05 | 0.306547 | -0.30797 |
15.56 | 0.023627 | 0.001251 | 0.254348 | -0.00097 | -0.00994 | -6E-05 | 0.303273 | -0.30424 |
19.5 | 0.022538 | 0.00116 | 0.253571 | -0.00037 | -0.00875 | -1.8E-05 | 0.301752 | -0.30212 |
24.0 | 0.022033 | 0.001167 | 0.252989 | -0.00018 | -0.00024 | 1E-06 | 0.300761 | -0.30095 |
The 19.5 million mesh is chosen considering accuracy and speed
#cells [m] | change [%] |
12.66 | - |
15.56 | 5.7 |
19.5 | 4.8 |
24.0 | 2.2 |
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FLOW SOLUTION
Y+ Distribution [19.5m mesh]
Pressure Distribution [19.5m mesh]
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STRUCTURAL PROPERTIES
T
L
H
Solid domain’s mesh is prepared structred. By changing the shown named parameters, different solid meshes are created.
These parameters stating the number of nodes used in that direction.
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STRUCTURAL SOLUTION
Size [L H T] | #Cells | Max Disp [mm] | Max VonMises [MPa] | Min VonMises [MPa] | Change [%] |
88-11-3 | 1740 | 16.45556 | 20.36163 | 8.2382e-4 | - |
110-14-3 | 2834 | 20.67708 | 23.73388 | 7.3453e-4 | 25.65 |
138-18-3 | 4658 | 24.41548 | 29.48812 | 5.1040e-4 | 18.07 |
172-22-3 | 7182 | 27.23301 | 34.52003 | 8.8937e-5 | 11.54 |
215-28-3 | 11556 | 29.96336 | 40.2692 | 3.9954e-6 | 10.03 |
270-35-3 | 18292 | 31.88641 | 45.62413 | 2.1788e-6 | 6.42 |
270-35-4 | 27438 | 32.59861 | 48.86389 | 2.9075e-6 | 2.23 |
340-45-4 | 44748 | 33.22963 | 51.02271 | 2.5936e-6 | 1.9 |
1kPa pressure difference is created between the top and bottom surfaces of the wing and displacement values obtained. The 270-35-4 [27438 cells] mesh is chosen considering speed and accuracy
SOLVER = ELASTICITY
GEOMETRIC_CONDITIONS = SMALL_DEFORMATIONS
MATERIAL_MODEL = LINEAR_ELASTIC
MATERIAL_COMPRESSIBILITY= COMPRESSIBLE
MATERIAL_DENSITY= 2700.0
ELASTICITY_MODULUS = 70E9
POISSON_RATIO = 0.33
FORMULATION_ELASTICITY_2D = PLANE_STRAIN
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STRUCTURAL SOLUTION
Displacement Magnitude [m]
VonMises Stress [Pa]
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FSI ANALYSIS
Fluid and structural solver settings are held similar to the previously shown analysis. Coupling is done throught the following configuration files:
coupled.cfg
SOLVER = MULTIPHYSICS CONFIG_LIST = (fluid.cfg, solid1.cfg, solid2.cfg)�MULTIZONE_SOLVER = BLOCK_GAUSS_SEIDEL OUTER_ITER = 20�KIND_INTERPOLATION = ISOPARAMETRIC CONSERVATIVE_INTERPOLATION = YES
DEFORM_STIFFNESS_TYPE = INVERSE_VOLUME DEFORM_LINEAR_SOLVER = CONJUGATE_GRADIENT
DEFORM_LINEAR_SOLVER_PREC = ILU DEFORM_NONLINEAR_ITER = 1
DEFORM_LINEAR_SOLVER_ITER = 10000 DEFORM_LINEAR_SOLVER_ERROR = 1E-14
DEFORM_CONSOLE_OUTPUT = YES MARKER_ZONE_INTERFACE = (wing1, wing1S_solid , wing2 , wing2S_solid)
solid1.cfg
MARKER_CLAMPED = ( wing1S_clamp)
MARKER_PRESSURE = ( wing1S_solid, 0)
MARKER_FLUID_LOAD = ( wing1S_solid )
MARKER_DEFORM_MESH = ( wing1S_solid )
solid2.cfg
MARKER_CLAMPED = ( wing2S_clamp)
MARKER_PRESSURE = ( wing2S_solid, 0)
MARKER_FLUID_LOAD = ( wing2S_solid )
MARKER_DEFORM_MESH = ( wing2S_solid )
fluid.cfg
MARKER_FLUID_LOAD = ( wing1,wing2)
DEFORM_MESH = YES
MARKER_DEFORM_MESH = ( wing1,wing2)
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FSI ANALYSIS
Wing1 | CFx | CFy | CFz | CMx | CMy | CMz |
Only Fluid | 0.010667 | 0.000256 | 0.126599 | 0.301752 | -0.004519 | -0.026704 |
FSI | 0.010706 | -0.00136 | 0.127518 | 0.303945 | -0.004358 | -0.02696 |
Difference | 3.9e-5 | -1.616e-3 | 9.19e-4 | 2.19e-3 | 1.61e-4 | -2.56e-4 |
Difference [%] | 0.3656 | -631.25* | 0.7259 | 0.7258 | -3.5627 | 0.9587 |
Wing2 | | |||||
Only Fluid | 0.011871 | 0.000904 | 0.126972 | -0.302123 | -0.004229 | 0.026686 |
FSI | 0.011894 | 0.002508 | 0.127302 | -0.304509 | -0.004063 | 0.02694 |
Difference | 2.3e-5 | 1.604e-3 | 3.3e-4 | -2.386e-3 | 1.66e-4 | 2.54e-4 |
Difference [%] | 0.1938 | 177.43* | 0.2599 | 0.7897 | -3.9252 | 0.9518 |
At the FSI equilibrium, change in the aerodynamic coefficients is observed.
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FSI ANALYSIS
Wing2 – [Orange] Original Geom – [Grey] Position after the FSI analysis
Displacement magnitude of the wings [m] / Top view
Wing1 – [Orange] Original Geom – [Grey] Position after the FSI analysis
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FFD BOX SETTINGS
FFD_TOLERANCE = 1E-10 DV_KIND = FFD_SETTING
FFD_ITERATIONS = 500 DV_MARKER = ( wing1 , wing2)
FFD_DEFINITION = (WINGBOX, -0.126, -1.03, -0.0577, 0.134, -1.03, … DV_VALUE = 0.0
DEFINITION_DV = ( 11, 1.0 | wing2 | WINGBOX, 0, 0, 0, 0.0 … FFD_DEGREE = (5, 21, 1)
DV_PARAM =( WINGBOX, 0, 0, 0, 0.0, 0.0, 1.0 ) FFD_CONTINUITY = 2ND_DERIVATIVE
Red points are fixed
To generate FFD Box, SU2DEF used with the modified config file, which has following additional settings
# Total Design Points = 264
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ADJOINT SOLUTION
The configuration file:
MATH_PROBLEM= CONTINUOUS_ADJOINT
OBJECTIVE_FUNCTION= DRAG
CONV_NUM_METHOD_ADJFLOW= JST
SLOPE_LIMITER_ADJFLOW= VENKATAKRISHNAN
ADJ_JST_SENSOR_COEFF= ( 0.0, 0.02 )
TIME_DISCRE_ADJFLOW= EULER_IMPLICIT
CFL_REDUCTION_ADJFLOW= 0.8
LIMIT_ADJFLOW= 1E6
SENS_REMOVE_SHARP = NO
SU2_CFD is used for solution.
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AN ODD PROBLEM
Oddly deformed fluid surface after mapping structural deformation with RBF
Changing settings did not solve the problem…
In between every rib surface, trailing edge become step like structure with ‘Y’ shape and every mid points between ribs and spars, surface becomed crippled/wavy with ISOPARAMETRIC.
Changing settings did not solve the problem…
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FUTURE WORK
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ADJOINT BASED AEROELASTIC SHAPE OPTIMIZATION OF A SLENDER WING MOUNTED ON A LOITERING MUNITION
Thank you for your attention…
Presented By : Emirhan Evin
E-mail : emirhan.evin@metu.edu.tr
5th Conference - 2024