Post on 09-Jan-2017
Efficient and Sensitive Energy Harvesting Using Piezoelectric Compliant Mechanisms
Xiaokun Ma*Hong Goo Yeo†
Christopher D. Rahn*Susan Trolier-McKinstry†
*Department of Mechanical and Nuclear Engineering†Department of Materials Science and Engineering
The Pennsylvania State University
August 4th 2015
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• Weak base excitation Low frequency (< 10 ) Low amplitude (< 1)
• Shock rather than vibration inputs Broad band (not tonal) frequency distribution Potential for damage due to large shocks
• Small footprint on the order of
• Fragile thin films and structures Shock inputs can damage structure Self limiting design for robust performance (bump stops or bridges)
Energy Harvesting from Human MotionHas Unique Challenges
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Acceleration
Wrist acceleration data during running(Lach, 2013, University of Virginia)
Dominant motion frequency of common human activities(Gorlatova, 2013, Columbia University)
Impulse-excited energy harvester(Pillatsch, 2012, Smart Materials and Structures)
Piezoelectric Energy Harvesting Devices
Bimorph cantilever with a tip proof mass(Erturk, 2009, Smart Materials and Structures)
Buckled slender bridges(Jung, 2010, Applied Physics Letters)
Alternative beam geometries(Roundy, 2005, Pervasive Computing)
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• Piezoelectric Compliant Mechanism (PCM) Design and Model
• PCM Quadratic Boundary Condition and Maximum Power Analysis
• Analysis Results (PZT)
• Experimental Results (PVDF)
• Conclusions and Future Work
Outline
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Impedance matching
Quadratic boundary condition
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PCM Design
No friction
Clamped => Reliable connection Bridge structure => Self-limiting design =>
Improve robustness
• Equation of motion
Boundary conditions:
Moment balance at : Shear balance at :
• Electrical circuit equation
Governing Equations
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Bending stiffness Mass
Strain rate damping
Air damping
Electrical coupling
Mechanical coupling
• Frequency domain model Transcendental transfer functions:
• Time domain model Eigenfunction:
Modal analysis:
PCM Model
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• Piezoelectric Compliant Mechanism (PCM) Design and Model
• PCM Quadratic Boundary Condition and Maximum Power Analysis
• Analysis Results (PZT)
• Experimental Results (PVDF)
• Conclusions and Future Work
Outline
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where , , and
PCM Quadratic Boundary ConditionUniform strain
throughout the PZTQuadratic
mode shapeShear force at is zeroMoment at is nonzero
must satisfy:
Boundary conditions at :
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Maximum Power Analysis• Mode shape efficiency
: obtained when the maximum strain in the PZT reaches its limit : obtained when the entire volume of the PZT is sinusoidally strained to its limit at a given
frequency
• Key assumptions Base excitation sinusoidally excites the structure at one frequency The entire PZT volume is uniformly strained to when excited by base acceleration at PZT is strained in 1 direction with field generated in the 3 direction ( mode) Load impedance is a resistor
Electrical circuit equation:𝐺 (𝑠)=
𝑉 (𝑠 )𝑆1(𝑠)
=𝐴h𝑝𝐸𝑝𝑑31𝑅𝑙 𝑠𝐴𝜀33
𝑆 𝑅𝑙 𝑠+h𝑝
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𝑆1 (𝑡 )=𝑆𝑙𝑖𝑚sin (𝜔𝑡 )𝑑𝑃𝑑𝑅 𝑙
=0
• Piezoelectric Compliant Mechanism (PCM) Design and Model
• PCM Quadratic Boundary Condition and Maximum Power Analysis
• Analysis Results (PZT)
• Experimental Results (PVDF)
• Conclusions and Future Work
Outline
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Frequency Domain Comparison
() ()Power
Sensitivity()
Max Strain Sensitivity
()(0.1% strain)
() ()Mode Shape
Efficiency
Proof Mass Cantilever 4.95 138 22.8 3.24% 21.7 106 20.5%
PCM 5.01 136 215 5.05% 84.3 107 78.6%
Voltage PowerRelative Tip Displacement
Proof Mass Cantilever
PCM
9x larger power
sensitivity
4x larger power with the same
maximum strain
4x higher mode shape
efficiency
Transcendental transfer functionState space model
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Time Domain ComparisonVoltage PowerTip Displacement
Proof Mass Cantilever
PCM
Wrist Acceleration During Running 1.75
10.7
Average Power() Running Jogging Walking
Proof Mass Cantilever 1.75 0.716 0.0247
PCM 10.7 3.60 0.0667
6x larger average power 13
• Piezoelectric Compliant Mechanism (PCM) Design and Model
• PCM Quadratic Boundary Condition and Maximum Power Analysis
• Analysis Results (PZT)
• Experimental Results (PVDF)
• Conclusions and Future Work
Outline
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Experimental Setup
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Tip Displacement Frequency Response
()Tip Displacement Sensitivity
()
Proof Mass Cantilever
Theory 5.22 0.179
Experiment 5.28 0.175
PCMTheory 5.02 0.0864
Experiment 5.13 0.0829
Proof Mass Cantilever PCM
Cantilever theoryCantilever experimentPCM theoryPCM experiment: optimal stiffness
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Voltage & Power Frequency Responses
Proof Mass Cantilever
PCM
Voltage Power
Cantilever theoryCantilever experimentPCM theoryPCM experiment: optimal stiffnessPCM experiment: lower stiffnessPCM experiment: higher stiffness 17
Mode Shape and Strain Distribution1st Mode Shape
Voltage Sensitivity
()
Power Sensitivity
()
Max Strain Sensitivity
()(1% Strain)
()(1% Strain)
() ()Mode Shape
Efficiency
Proof Mass Cantilever
Theory 154 4.50 3.29% 46.8 0.416 1.75 23.8%
Experiment 136 3.53 3.52% 38.6 0.285 16.3%
PCMTheory 90.5 1.56 1.05% 86.2 1.41 1.68 84.2%
Experiment 80.8 1.24 1.01% 80.0 1.22 72.4%
2x larger voltage with the same
maximum strain
4x larger power with the same
maximum strain
4x higher mode shape efficiency
Strain Distribution
Cantilever theoryCantilever experimentPCM theoryPCM experiment: optimal stiffnessPCM experiment: lower stiffnessPCM experiment: higher stiffness
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• Piezoelectric Compliant Mechanism (PCM) Design and Model
• PCM Quadratic Boundary Condition and Maximum Power Analysis
• Analysis Results (PZT)
• Experimental Results (PVDF)
• Conclusions and Future Work
Outline
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Conclusions and Future Work
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• Conclusions The PCM energy harvester can harvest energy within the bandwidth of human movement
without a large proof mass Careful stiffness tuning enforces a PCM quadratic boundary condition, making the PCM first
mode shape closer to a parabola and more efficient The PCM has 9 times higher power sensitivity at resonance and 6 times higher average power
in response to realistic base excitation input than the proof mass cantilever at the same damping ratio
The PCM generates twice more voltage and 4 times more power than the proof mass cantilever with the same maximum strain
The PCM improves mode shape efficiency by 4 times, from 20% to 80%
• Future Work Study the nonlinear effect of the PCM energy harvester under large base excitation Investigate the PCM energy harvester with an initially-curved or pre-buckled piezoelectric
beam
Thank you!21
• Acknowledgment The authors thank Shanshan Chen and Dr. John Lach in the University of Virginia for providing
the wrist acceleration data The authors thank Andrew Wilson for the help in the PCM energy harvester fabrication This work was supported by the National Science Foundation ASSIST Nanosystems ERC
under Award Number EEC-1160483