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Setup and Validation of High Fidelity
Aeroelastic Analysis Methods Based
on RBF Mesh Morphing
Ubaldo Cella
Rome 27 March 2017
Supervisor : Prof. Marco Evangelos Biancolini
Coordinator : Prof. Roberto Montanari
Rome 27 March 2017Ubaldo Cella
Research framework
Rome 27 March 2017Ubaldo Cella
High fidelity FSI analyses
CFD
FEM
Rome 27 March 2017Ubaldo Cella
Overview of the work
• Setup of FSI analysis methods
• 2-way (CFD-CSM) coupling
• Modal approach for aeroelastic analyses
• Validation against experiments
• Piaggio P1XX aircraft (transonic)
• RIBES wing (subsonic)
Rome 27 March 2017Ubaldo Cella
2 ways FSI procedure
CFD
computation
Loads
mapping
FEM
computation
CFD Mesh
updating
Deformed
shape
Shape
changed?
Undeformed
geometry
END
Yes No
Rome 27 March 2017Ubaldo Cella
Mesh morphing
Rome 27 March 2017Ubaldo Cella
RBF Morph tool
• Setup
• Select fixed and
moving walls by source
points
• Prescribe the
displacements (or a
combination of)
• Fitting
• Solving the RBF system
and storing the solution
• Smoothing
• Application of the
morphing action on
surfaces and volume
Rome 27 March 2017Ubaldo Cella
Modal approach for FSI
Structural modal analysis
Morphed CFD mesh database (one per mode)
Parametric mesh update
Modal coordinates
Convergence?
Undeformed geometry
END
No
Yes
CFD iterations
CFD
flexible
model
= +
modal coordinate
nodal modes
displacement
number of
natural modes
Parametric mesh formulation
Rome 27 March 2017Ubaldo Cella
Advantages and limits
• Main advantages
• simpler numerical environments respect 2-way
• Higher robustness
• Mesh adaptation during computation (faster
solution)
• Limits
• Linear problems only (small displacements)
• Uncertainness on the modal base dimension
Rome 27 March 2017Ubaldo Cella
Piaggio P1XX
Rome 27 March 2017Ubaldo Cella
Computational domains
CFD mesh
structured 14 mill. Cells
FEM mesh
28.000 hexa elementsfully steel-made
Rome 27 March 2017Ubaldo Cella
RBF problem setup
2 steps mesh morphing procedure
Rome 27 March 2017Ubaldo Cella
2-ways convergence hist.
Undef. 1 2 3
Iteration
CL
CL = 0.005
Undef. 1 2 3
Iteration
CD
CD = 2 dc
~1% of the wing
exposed semispan
(figure amplified)
Rome 27 March 2017Ubaldo Cella
Modal shapes
Modal base composed with up to 6 modes
Rome 27 March 2017Ubaldo Cella
CL
α
α = 0.1 deg
Solutions comparison
CL
CD
Exp.
Undef.
2-ways
1 mode
2 modes
3 modes
4 modes
5 modes
6 modes
CL = 0.01
CD = 2 dc
Mach 0.8
Rome 27 March 2017Ubaldo Cella
Aero-structure coupling
Flow direction
Elastic axis
Surface pressure
Rome 27 March 2017Ubaldo Cella
Pressure comparison
Rome 27 March 2017Ubaldo Cella
RIBES wing
Rome 27 March 2017Ubaldo Cella
Critical points of design
• Challenging structural similitude with a real
full scale wing
• Impracticable manufacturing
• Conflicting high deformation requirement
• Relatively higher thickness and lower loads
• Difficult to load the spars and unload the skin
• Panels stability was the main design driver
• Manufacturing requirements defined on
progress
• Several iteration with the model manufacturer
Rome 27 March 2017Ubaldo Cella
Final test article details
Span = 1.6 m
Material = AL2024T3 (Yeld Stress = 270 Mpa, Ultimate stress = 440 Mpa)
Rome 27 March 2017Ubaldo Cella
Pressure taps installation
80 pressure taps
Rome 27 March 2017Ubaldo Cella
Strain gauges installation
3 rosettes (three channels)
16 unidirectional
Rome 27 March 2017Ubaldo Cella
Model under construction
Rome 27 March 2017Ubaldo Cella
Measured geometry
model measured
by HEXAGON
metrology
electronic harm
measured
Rome 27 March 2017Ubaldo Cella
Effects on aerodynamics
-2
-1.5
-1
-0.5
0
0.5
1
1.5
0 0.2 0.4 0.6 0.8 1
Cp Alfa 5 deg
Measured
Nominal
Rome 27 March 2017Ubaldo Cella
CAD reconstruction
Rome 27 March 2017Ubaldo Cella
Free flight CFD domain
C-H structured 3.2 mill. Hexa, farfield at 50 MAC
Rome 27 March 2017Ubaldo Cella
Structural model
97000 shell elements
Rome 27 March 2017Ubaldo Cella
Modal shapes
Rome 27 March 2017Ubaldo Cella
RBF problem domain
31000 source points, (fitting in 62 sec.,
smoothing in 40 sec.)
Rome 27 March 2017Ubaldo Cella
Aerodynamic solutions
CFD with rigid
model (no elasticity
accounted)
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
-5 0 5 10 15
CL
α
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
0 0.02 0.04 0.06 0.08
CL
CD
CFD
Experiments
Rome 27 March 2017Ubaldo Cella
Deformation measurement
High-precision
inclinometer
Rome 27 March 2017Ubaldo Cella
Deformation solutions
0
1
2
3
4
5
6
7
8
9
0 400 800 1200 1600
Δz,mm
y, mm
Measurements
Δz 2-way
Δz 8modes
-0.002
0
0.002
0.004
0.006
0.008
1 2 3 4 5 6 7 8
Mode
Modal coordinate
Rome 27 March 2017Ubaldo Cella
Elements junction
Rome 27 March 2017Ubaldo Cella
FEM verification
Exp. σy = -15.6 MPa
FEM σy = ∼ -38 MPa
Exp. σy = -143.2 MPa
FEM σy = ∼ -21 MPa
Rome 27 March 2017Ubaldo Cella
Spar reinforcements
Rome 27 March 2017Ubaldo Cella
Conclusions
• RBF morphing provide a very efficient and
robust coupling of CFD and FEM solutions
• 2-way and modal FSI analyses provided
almost the same solutions
• the modal approach is a valid candidate to setup
efficient and accurate FSI analyses of wings
• A very poorly populated modal base us sufficient
for lifting surfaces
• Failure in modeling the load shared between
skin and spar.
• A more accurate FEM model is probably necessary
for complex topologies including root junctions
Rome 27 March 2017Ubaldo Cella
Future work
• Unsteady dynamic FSI implementation to
study complex phenomena as flutter or
buffet.
• Validation against dynamic test cases
• HiReNASD ?
• AGARD 445.6 ?
• Extension of RIBES model tests?
• Sails ?
Setup and Validation of High Fidelity Aeroelastic Analysis Methods Based on RBF Mesh Morphing

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Setup and Validation of High Fidelity Aeroelastic Analysis Methods Based on RBF Mesh Morphing

  • 1. Setup and Validation of High Fidelity Aeroelastic Analysis Methods Based on RBF Mesh Morphing Ubaldo Cella Rome 27 March 2017 Supervisor : Prof. Marco Evangelos Biancolini Coordinator : Prof. Roberto Montanari
  • 2. Rome 27 March 2017Ubaldo Cella Research framework
  • 3. Rome 27 March 2017Ubaldo Cella High fidelity FSI analyses CFD FEM
  • 4. Rome 27 March 2017Ubaldo Cella Overview of the work • Setup of FSI analysis methods • 2-way (CFD-CSM) coupling • Modal approach for aeroelastic analyses • Validation against experiments • Piaggio P1XX aircraft (transonic) • RIBES wing (subsonic)
  • 5. Rome 27 March 2017Ubaldo Cella 2 ways FSI procedure CFD computation Loads mapping FEM computation CFD Mesh updating Deformed shape Shape changed? Undeformed geometry END Yes No
  • 6. Rome 27 March 2017Ubaldo Cella Mesh morphing
  • 7. Rome 27 March 2017Ubaldo Cella RBF Morph tool • Setup • Select fixed and moving walls by source points • Prescribe the displacements (or a combination of) • Fitting • Solving the RBF system and storing the solution • Smoothing • Application of the morphing action on surfaces and volume
  • 8. Rome 27 March 2017Ubaldo Cella Modal approach for FSI Structural modal analysis Morphed CFD mesh database (one per mode) Parametric mesh update Modal coordinates Convergence? Undeformed geometry END No Yes CFD iterations CFD flexible model = + modal coordinate nodal modes displacement number of natural modes Parametric mesh formulation
  • 9. Rome 27 March 2017Ubaldo Cella Advantages and limits • Main advantages • simpler numerical environments respect 2-way • Higher robustness • Mesh adaptation during computation (faster solution) • Limits • Linear problems only (small displacements) • Uncertainness on the modal base dimension
  • 10. Rome 27 March 2017Ubaldo Cella Piaggio P1XX
  • 11. Rome 27 March 2017Ubaldo Cella Computational domains CFD mesh structured 14 mill. Cells FEM mesh 28.000 hexa elementsfully steel-made
  • 12. Rome 27 March 2017Ubaldo Cella RBF problem setup 2 steps mesh morphing procedure
  • 13. Rome 27 March 2017Ubaldo Cella 2-ways convergence hist. Undef. 1 2 3 Iteration CL CL = 0.005 Undef. 1 2 3 Iteration CD CD = 2 dc ~1% of the wing exposed semispan (figure amplified)
  • 14. Rome 27 March 2017Ubaldo Cella Modal shapes Modal base composed with up to 6 modes
  • 15. Rome 27 March 2017Ubaldo Cella CL α α = 0.1 deg Solutions comparison CL CD Exp. Undef. 2-ways 1 mode 2 modes 3 modes 4 modes 5 modes 6 modes CL = 0.01 CD = 2 dc Mach 0.8
  • 16. Rome 27 March 2017Ubaldo Cella Aero-structure coupling Flow direction Elastic axis
  • 18. Rome 27 March 2017Ubaldo Cella Pressure comparison
  • 19. Rome 27 March 2017Ubaldo Cella RIBES wing
  • 20. Rome 27 March 2017Ubaldo Cella Critical points of design • Challenging structural similitude with a real full scale wing • Impracticable manufacturing • Conflicting high deformation requirement • Relatively higher thickness and lower loads • Difficult to load the spars and unload the skin • Panels stability was the main design driver • Manufacturing requirements defined on progress • Several iteration with the model manufacturer
  • 21. Rome 27 March 2017Ubaldo Cella Final test article details Span = 1.6 m Material = AL2024T3 (Yeld Stress = 270 Mpa, Ultimate stress = 440 Mpa)
  • 22. Rome 27 March 2017Ubaldo Cella Pressure taps installation 80 pressure taps
  • 23. Rome 27 March 2017Ubaldo Cella Strain gauges installation 3 rosettes (three channels) 16 unidirectional
  • 24. Rome 27 March 2017Ubaldo Cella Model under construction
  • 25. Rome 27 March 2017Ubaldo Cella Measured geometry model measured by HEXAGON metrology electronic harm measured
  • 26. Rome 27 March 2017Ubaldo Cella Effects on aerodynamics -2 -1.5 -1 -0.5 0 0.5 1 1.5 0 0.2 0.4 0.6 0.8 1 Cp Alfa 5 deg Measured Nominal
  • 27. Rome 27 March 2017Ubaldo Cella CAD reconstruction
  • 28. Rome 27 March 2017Ubaldo Cella Free flight CFD domain C-H structured 3.2 mill. Hexa, farfield at 50 MAC
  • 29. Rome 27 March 2017Ubaldo Cella Structural model 97000 shell elements
  • 30. Rome 27 March 2017Ubaldo Cella Modal shapes
  • 31. Rome 27 March 2017Ubaldo Cella RBF problem domain 31000 source points, (fitting in 62 sec., smoothing in 40 sec.)
  • 32. Rome 27 March 2017Ubaldo Cella Aerodynamic solutions CFD with rigid model (no elasticity accounted) -0.2 0 0.2 0.4 0.6 0.8 1 1.2 -5 0 5 10 15 CL α -0.2 0 0.2 0.4 0.6 0.8 1 1.2 0 0.02 0.04 0.06 0.08 CL CD CFD Experiments
  • 33. Rome 27 March 2017Ubaldo Cella Deformation measurement High-precision inclinometer
  • 34. Rome 27 March 2017Ubaldo Cella Deformation solutions 0 1 2 3 4 5 6 7 8 9 0 400 800 1200 1600 Δz,mm y, mm Measurements Δz 2-way Δz 8modes -0.002 0 0.002 0.004 0.006 0.008 1 2 3 4 5 6 7 8 Mode Modal coordinate
  • 35. Rome 27 March 2017Ubaldo Cella Elements junction
  • 36. Rome 27 March 2017Ubaldo Cella FEM verification Exp. σy = -15.6 MPa FEM σy = ∼ -38 MPa Exp. σy = -143.2 MPa FEM σy = ∼ -21 MPa
  • 37. Rome 27 March 2017Ubaldo Cella Spar reinforcements
  • 38. Rome 27 March 2017Ubaldo Cella Conclusions • RBF morphing provide a very efficient and robust coupling of CFD and FEM solutions • 2-way and modal FSI analyses provided almost the same solutions • the modal approach is a valid candidate to setup efficient and accurate FSI analyses of wings • A very poorly populated modal base us sufficient for lifting surfaces • Failure in modeling the load shared between skin and spar. • A more accurate FEM model is probably necessary for complex topologies including root junctions
  • 39. Rome 27 March 2017Ubaldo Cella Future work • Unsteady dynamic FSI implementation to study complex phenomena as flutter or buffet. • Validation against dynamic test cases • HiReNASD ? • AGARD 445.6 ? • Extension of RIBES model tests? • Sails ?