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© Fraunhofer LBF
ENHANCED LIGHTWEIGHT DESIGN BY COMPOSITES –
RESULTS OF THE PROJECT ENLIGHT
Dirk Mayer, Thilo Bein, Hendrik Buff, Benedict Götz, Oliver Schwarzhaupt , Dominik Spancken
offenSeite 1
© Fraunhofer LBF
ENHANCED LIGHTWEIGHT DESIGN BY COMPOSITES –
RESULTS OF THE PROJECT ENLIGHT
Dirk Mayer, Thilo Bein, Hendrik Buff, Benedict Götz, Oliver Schwarzhaupt , Dominik Spancken
offenSeite 2
© Fraunhofer LBF
Lightweight Design as an Enabler for Future Mobility
 Decreased vehicle weight…
 Reduces energy consumption
 Less CO2 emission for
combustion engines
 Extended range for electric
vehicles
 Compensates for the added mass
by integration of batteries and
electronics into electric vehicles
 Reduces consumption of ressources
by using less
material
Relaxed
structural
design
requirements
Less motor
power
required
Smaller
battery
required
Reduced
battery mass
Reduced
structural
loads
„Lightweight spiral“, after FOREL - Chancen und Herausforderungen im ressourceneffizienten
Leichtbau für die Elektromobilität 2015// paulbr75, pixabay.com
© Fraunhofer LBF
Aims of the ENLIGHT project
Seite 4
© Fraunhofer LBF
Control Arm: The design conflict
Seite 5
Function Requirement
Connect the
wheel to the
chassis
High durability
Handling High stiffness
Low mass
Ride comfort:
Vibration
isolation
High Mass
Low stiffness
Original Golf V part:
4kg mass, steel
© Fraunhofer LBF
Lightweight NVH optimization by functional integration
Seite 6
 Tuned Mass Damper
 traditional tool for damping of
structural resonances
 Mechanical oscillator with a
sprung mass tuned to the host
resonance
 Added mass: 5-20% of the
effective host mass
 Shunt Damping
 Integration of piezo elements
(electromechanical transducers)
 Inductive shunting: electromechanical oscillator
 TMD effect without added mechanical inertial masses
 Might be realised by passive components (semi-active
system)
© Fraunhofer LBF
Potential performance of semi-active damping
 Main driver for the performance of shunt
damping:
 Generalized electromechanical coupling
coefficient:
 𝑘𝑘𝑖𝑖𝑖𝑖 =
𝜔𝜔𝑛𝑛𝑛𝑛
2 −𝜔𝜔𝑛𝑛𝑆𝑆
2
𝜔𝜔𝑛𝑛𝑛𝑛
2
 GEMCC is influenced by:
 Electromechanic coupling of the material
 Stiffness of the piezo material
 Position of the piezo w/r to the eigenmodes
Seite 7
Hollkamp, J. J.; Starchville, T. F. (1994): A Self-Tuning Piezoelectric Vibration Absorber. In:
Journal of Intelligent Material Systems and Structures 5 (4), S. 559–566. DOI:
10.1177/1045389X9400500412.
© Fraunhofer LBF
Design of vibration control systems – passive and semi-active
Seite 8
 Concurrent design considering mechanical stiffness and dynamic properties
 Integration of piezoelectric elements into the structural design
Baseline structure
 Stiffness k
(design requirements)
 Mass M
 Vibrations at
resonance frequency
M
F
x
1) Initial structure
+ Vibration Absorber
 Stiffness k
 Lower vibrations
 Higher mass
M + M_TVA
MTVA
2) TMD solution
+ Mounted piezo
elements
 Lower vibrations
 Higher mass
M + M_piezo
 Higher stiffness due
to piezo
(overengineered)
Mpiezo
3) Retrofitting of piezos
Integrated piezo elements
 Consider piezo
stiffness in the design
 Stiffnes optimized
 Lower vibrations
 Additional mass
reduced
4) Integrated design
© Fraunhofer LBF
CFRP Control Arm
Seite 9
 Woven fiber layers reinforced by uni-directional (DU) tapes
Al / Plastic Insert
Bolt
Laminate
 Bolted aluminum connectors to chassis and wheel
© Fraunhofer LBF
Integration of Piezoelectric elements
Seite 10
 Design procedure:
 Numerical analyses  Structural resonances and respective strain modes  piezo position
 Iterative optimization of GEMCC by changing piezo geometry
 Model order reduction and shunt circuit optimization
© Fraunhofer LBF
Optimization results
Initial CFRP part Optimized CFRP part
Smart Structure
(CFRP part + piezo
module)
Lateral stiffness [kn/mm] 219,9 182,0 186,2
Long. Stiffness [kn/mm] 9,906 8,400 9,979
1st resonance [Hz] 62,95 57,92 62,98
Mass [kg] (without fittings) 0,644 0,540 0,600
Seite 11
Mass of aluminum fittings ~1.5 kg  50% mass reduction with respect to the steel part
© Fraunhofer LBF
Comparison with a TMD solution
Seite 12
 Numerical simulation of a reduced order model
 CFRP part plus 22,5 kg rigid mass (wheel, hub, brakes)
 GEMCC = 0.07
 Shunt circuit enhanced by an active negative capacitance
 TMD at the wheel hub, m = 1,6 kg
© Fraunhofer LBF
Manufacturing of a prototype
 Hand lamination
 Stack of 18 PZT transducers DuraAct P-876.A11(50 mm x 30 mm x 100 µm)
 Design changes due to practical reasons: Thinner piezos, application to the inner side of the control arm
 Integration of fibre-optical sensing for monitoring of strains
Seite 13
Piezostack
© Fraunhofer LBF
Dynamic analyses in the laboratory
 Free boundary conditions
 Shaker excitation
 Laser Doppler vibrometer for response
measurements
Seite 14
© Fraunhofer LBF
Result
 First resonance at 195Hz
 No frequency shift detectable between open
and short circuited piezos
 Electromechanical coupling very low
 About 6dB reduction
 Less than predicted in the simulation
Seite 15
© Fraunhofer LBF
Durability Testing: Structural stiffness
 Uni-axial cyclic load test
 Load program derived from design loads
 Small loss of stiffness during cyclic testing
 Control arm fails at 200% of the
design load
Seite 16
© Fraunhofer LBF
Durability Testing: Analysis of Piezo Transducers
 Impedance analysis
 0 cycles
 200k cycles
 402k cycles
 No significant changes in the measured
impedance
 Durable coupling to the structure
 Durable stacking and electrical
connection
Seite 17
0 1 2 3 4 5 6 7 8 9 10
x 10
4
10
-1
10
0
10
1
10
2
frequency [Hz]
realImpedance[Ω]
0 1 2 3 4 5 6 7 8 9 10
x 10
4
0
0.5
1
1.5
frequency [Hz]
imagAdmittance[Ω-1]
baseline
after 200,000 cycles
after 402,000 cycles
baseline
after 200,000 cycles
after 402,000 cycles
© Fraunhofer LBF
Conclusions
 Integration of semi-active damping with piezos into highly loaded, stiff components is possible
 Concurrent design approach is feasible
 Function integration should be already considered in the early conceptual design stage
 Manufacturing issues should be integrated into the simulation
 Realistic testing of smart structures in the laboratory as an own research topic for future projects
Seite 18

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Presentation IMTC 2017

  • 1. © Fraunhofer LBF ENHANCED LIGHTWEIGHT DESIGN BY COMPOSITES – RESULTS OF THE PROJECT ENLIGHT Dirk Mayer, Thilo Bein, Hendrik Buff, Benedict Götz, Oliver Schwarzhaupt , Dominik Spancken offenSeite 1
  • 2. © Fraunhofer LBF ENHANCED LIGHTWEIGHT DESIGN BY COMPOSITES – RESULTS OF THE PROJECT ENLIGHT Dirk Mayer, Thilo Bein, Hendrik Buff, Benedict Götz, Oliver Schwarzhaupt , Dominik Spancken offenSeite 2
  • 3. © Fraunhofer LBF Lightweight Design as an Enabler for Future Mobility  Decreased vehicle weight…  Reduces energy consumption  Less CO2 emission for combustion engines  Extended range for electric vehicles  Compensates for the added mass by integration of batteries and electronics into electric vehicles  Reduces consumption of ressources by using less material Relaxed structural design requirements Less motor power required Smaller battery required Reduced battery mass Reduced structural loads „Lightweight spiral“, after FOREL - Chancen und Herausforderungen im ressourceneffizienten Leichtbau für die Elektromobilität 2015// paulbr75, pixabay.com
  • 4. © Fraunhofer LBF Aims of the ENLIGHT project Seite 4
  • 5. © Fraunhofer LBF Control Arm: The design conflict Seite 5 Function Requirement Connect the wheel to the chassis High durability Handling High stiffness Low mass Ride comfort: Vibration isolation High Mass Low stiffness Original Golf V part: 4kg mass, steel
  • 6. © Fraunhofer LBF Lightweight NVH optimization by functional integration Seite 6  Tuned Mass Damper  traditional tool for damping of structural resonances  Mechanical oscillator with a sprung mass tuned to the host resonance  Added mass: 5-20% of the effective host mass  Shunt Damping  Integration of piezo elements (electromechanical transducers)  Inductive shunting: electromechanical oscillator  TMD effect without added mechanical inertial masses  Might be realised by passive components (semi-active system)
  • 7. © Fraunhofer LBF Potential performance of semi-active damping  Main driver for the performance of shunt damping:  Generalized electromechanical coupling coefficient:  𝑘𝑘𝑖𝑖𝑖𝑖 = 𝜔𝜔𝑛𝑛𝑛𝑛 2 −𝜔𝜔𝑛𝑛𝑆𝑆 2 𝜔𝜔𝑛𝑛𝑛𝑛 2  GEMCC is influenced by:  Electromechanic coupling of the material  Stiffness of the piezo material  Position of the piezo w/r to the eigenmodes Seite 7 Hollkamp, J. J.; Starchville, T. F. (1994): A Self-Tuning Piezoelectric Vibration Absorber. In: Journal of Intelligent Material Systems and Structures 5 (4), S. 559–566. DOI: 10.1177/1045389X9400500412.
  • 8. © Fraunhofer LBF Design of vibration control systems – passive and semi-active Seite 8  Concurrent design considering mechanical stiffness and dynamic properties  Integration of piezoelectric elements into the structural design Baseline structure  Stiffness k (design requirements)  Mass M  Vibrations at resonance frequency M F x 1) Initial structure + Vibration Absorber  Stiffness k  Lower vibrations  Higher mass M + M_TVA MTVA 2) TMD solution + Mounted piezo elements  Lower vibrations  Higher mass M + M_piezo  Higher stiffness due to piezo (overengineered) Mpiezo 3) Retrofitting of piezos Integrated piezo elements  Consider piezo stiffness in the design  Stiffnes optimized  Lower vibrations  Additional mass reduced 4) Integrated design
  • 9. © Fraunhofer LBF CFRP Control Arm Seite 9  Woven fiber layers reinforced by uni-directional (DU) tapes Al / Plastic Insert Bolt Laminate  Bolted aluminum connectors to chassis and wheel
  • 10. © Fraunhofer LBF Integration of Piezoelectric elements Seite 10  Design procedure:  Numerical analyses  Structural resonances and respective strain modes  piezo position  Iterative optimization of GEMCC by changing piezo geometry  Model order reduction and shunt circuit optimization
  • 11. © Fraunhofer LBF Optimization results Initial CFRP part Optimized CFRP part Smart Structure (CFRP part + piezo module) Lateral stiffness [kn/mm] 219,9 182,0 186,2 Long. Stiffness [kn/mm] 9,906 8,400 9,979 1st resonance [Hz] 62,95 57,92 62,98 Mass [kg] (without fittings) 0,644 0,540 0,600 Seite 11 Mass of aluminum fittings ~1.5 kg  50% mass reduction with respect to the steel part
  • 12. © Fraunhofer LBF Comparison with a TMD solution Seite 12  Numerical simulation of a reduced order model  CFRP part plus 22,5 kg rigid mass (wheel, hub, brakes)  GEMCC = 0.07  Shunt circuit enhanced by an active negative capacitance  TMD at the wheel hub, m = 1,6 kg
  • 13. © Fraunhofer LBF Manufacturing of a prototype  Hand lamination  Stack of 18 PZT transducers DuraAct P-876.A11(50 mm x 30 mm x 100 µm)  Design changes due to practical reasons: Thinner piezos, application to the inner side of the control arm  Integration of fibre-optical sensing for monitoring of strains Seite 13 Piezostack
  • 14. © Fraunhofer LBF Dynamic analyses in the laboratory  Free boundary conditions  Shaker excitation  Laser Doppler vibrometer for response measurements Seite 14
  • 15. © Fraunhofer LBF Result  First resonance at 195Hz  No frequency shift detectable between open and short circuited piezos  Electromechanical coupling very low  About 6dB reduction  Less than predicted in the simulation Seite 15
  • 16. © Fraunhofer LBF Durability Testing: Structural stiffness  Uni-axial cyclic load test  Load program derived from design loads  Small loss of stiffness during cyclic testing  Control arm fails at 200% of the design load Seite 16
  • 17. © Fraunhofer LBF Durability Testing: Analysis of Piezo Transducers  Impedance analysis  0 cycles  200k cycles  402k cycles  No significant changes in the measured impedance  Durable coupling to the structure  Durable stacking and electrical connection Seite 17 0 1 2 3 4 5 6 7 8 9 10 x 10 4 10 -1 10 0 10 1 10 2 frequency [Hz] realImpedance[Ω] 0 1 2 3 4 5 6 7 8 9 10 x 10 4 0 0.5 1 1.5 frequency [Hz] imagAdmittance[Ω-1] baseline after 200,000 cycles after 402,000 cycles baseline after 200,000 cycles after 402,000 cycles
  • 18. © Fraunhofer LBF Conclusions  Integration of semi-active damping with piezos into highly loaded, stiff components is possible  Concurrent design approach is feasible  Function integration should be already considered in the early conceptual design stage  Manufacturing issues should be integrated into the simulation  Realistic testing of smart structures in the laboratory as an own research topic for future projects Seite 18