micro/nano mechanical systems lab –class#5 · finger motions (chip-size), footsteps (palm-size)...
TRANSCRIPT
Microsystems LaboratoryUC-Berkeley, ME Dept.
1Liwei Lin, University of California at Berkeley
Micro/Nano Mechanical Systems Lab – Class#5
Liwei Lin
Professor, Dept. of Mechanical Engineering Co-Director, Berkeley Sensor and Actuator CenterThe University of California, Berkeley, CA94720
e-mail: [email protected]://www.me.berkeley.edu/~lwlin
Microsystems LaboratoryUC-Berkeley, ME Dept.
2Liwei Lin, University of California at Berkeley
Outline
Review – Energy Harvesters Intro - MicroRobots
Microsystems LaboratoryUC-Berkeley, ME Dept.Power Sources for
Electronics & Sensors in IoT ?
“IoT will consist of almost 50 billion objects by 2020”.—— Dave Evans, Cisco
2020
1. Sensors2. Power3. Wireless Comm.
Microsystems LaboratoryUC-Berkeley, ME Dept.
Energy from Mechanical SourcesThere are many available mechanical energy sources in the real world, ranging from human motion, water falls, ocean waves, bridge/building/train motion, wind, cars, sound/acoustics … There have been several research reports on mechanical energy harvesters.Source Frequency Generated Power Reference/Source
Human Motion
<5 Hz ~100 W for a 65 kg Man 1. Wang, Z. et al. ACS Nano 2013, 9533.2. Brooks, G. et al. Exercise Physiology: Human Bioenergetics and Its Applications. McGraw-Hill, ,2005
Water Drop/Rain
<5 Hz 20 MJ or 5.5 kWh for 1000 kg form 2000 m
3. Lin, Z. et al. Angew. Chem. Int. Edi. 2013, 125, 12777.4.http://large.stanford.edu/courses/2010/ph240/harting2/
Ocean Waves
<10Hz 2,640 TWh/Year All Around the Word
5. Zi, Y. et al. ACS Nano, 2016, 10, 4797. 6. https://www.boem.gov/Ocean-Wave-Energy/
Bridge/building
1-40 Hz Acceleration from 0.01 to 3.8g; Power Density 0.01 to 9539 μW/cm3
7. Abu Riduan, M. et al. J. Semicond. 2012, 33, 074001.8. Khan, F. et al. Shock and Vibration, 2016, 1340402.
Train/Rail <20 Hz ~ 2.5 mW/cm3 for a 120 km/h Train
9. Jin, L. et al, Nano Energy, 2017, 38, 185.10. Paul, C. et al. J. Bridge. Eng. 19. 04014034.
Air Flow/Wind
<100 Hz ~ 800 TWh/Year All Around the Word
11. Wang, Z. et al, Angew. Chem. Int. Edi. 2012, 51, 11700.12. https://en.wikipedia.org/wiki/Wind_power
Vehicle Engine
<300 Hz 0.1-1 mW/cm2 for a Honda Car
13. Yang, J. et al, IEEE T. Contr. Syst. T. 2001, 9 (2), 295.14. Chen, J. Et al. Adv. Mater. 2013, 25, 6094.
Sound/Acoustic Noise
20 Hz-20 kHz
0.003 μW/cm2 for 75 dB0.96 μW/cm2 for 100 dB
15. https://en.wikipedia.org/wiki/Audio_frequency16. Yildiz, F. J. Tech. Study, 2009, 35, 40.
Microsystems LaboratoryUC-Berkeley, ME Dept.Example: Human Motions
There are significant mechanical energy sources available for harvesting in human activities using different sizes for optimal energy collections, such as: finger motions (chip-size), footsteps (palm-size) and body motions (large size) using potential various energy conversion mechanisms, including piezoelectric, triboelectric, electrets …
Human Motion Generated Mechanical Power
Ideal Converted Electrical Power
Ideal Converted Electrical Energy
Blood Flow 0.93 W 0.16 W 0.16 JExpiration 1 W 0.17 W 1.02 JBreathing 0.83 W 0.14 W 0.84 JUpper Limb Motion 60 W 10-30 W 10.2 JFinger Motion 6.9-19 mW 1.2-3.3 mW 226-406 μJWalking Motion 67 W 11-39 W 18.6 J
chip
chippalm/large
Palm/largelarge
chip
Microsystems LaboratoryUC-Berkeley, ME Dept.MEMS Integrated Harvesters
Dev
ice
Size
Peak Output Power
cm2
mm2
nWPiezoelectric
Chip-scale Integrated
Integrated Sensors
Integrated Circuits
1. Integrated CMOS process2. High volume low cost fabrication3. Materials & process development4. Design & application demos
W
Microsystems LaboratoryUC-Berkeley, ME Dept.
Fully CMOS Integrated Process
p+p+
N well
SiO 2
SiO 2 SiO 2p+ Poly
Top Electrode
SiO 2
Passivation layer
Opening
Energy Harvester(Mo/AlN/Mo)
Si-substrate
Bottom Electrode
Proof Mass
Piezoelectric Material (AlN)
“Beyond Microelectronics”Current state-of-art microelectronics are powered by external power sources. On-chip power sources such as MEMS energy harvesters can extend the chips to another dimension beyond the current capabilities. CMOS is the most widely utilized process to be utilized here.
Material and Process - I
Microsystems LaboratoryUC-Berkeley, ME Dept.Material and Process - II
Multilayered piezoelectric flexible energy harvester using interleaved electrodes a. Multiple layers of 20 µm piezoelectric polymer (e.g., P(VDF-TrFE)) sandwiched with metal electrodesb. Development of novel piezoelectric polymer with additives to form polar phase with enhanced piezoelectricityc. Enhanced output power by electrically parallel-connection and impedance matched designd. Low-temperature, low-cost and scalable process for IOT applications
Microsystems LaboratoryUC-Berkeley, ME Dept.
Flexible Piezoelectric TransducerPart I:
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Microsystems LaboratoryUC-Berkeley, ME Dept.
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Piezoelectricity
Active Effect
Negative EffectQuartz
Electrical Dipoles
Piezoelectric Effect is the ability of certain materials to generate an electric charge in response to applied mechanical stress.
Microsystems LaboratoryUC-Berkeley, ME Dept.Piezoelectric Materials
Single Crystal materials: Zinc Oxide (ZnO), Quartz, Barium Titanate (BaTiO3), etc.Polycrystal materials: There is no piezoelectricity before poling. Piezoceramics (PZT), Piezopolymers (PVDF), etc.
E
Before poling In poling After poling
I II III
Electrical Poling: Applying high electrical field to dipoles
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Microsystems LaboratoryUC-Berkeley, ME Dept.
Example: ZnO Nanowires
Z. L. Wang, J. Song, Science 2006, 312, 242. 12
Microsystems LaboratoryUC-Berkeley, ME Dept.
Transport is governed by a metal-semiconductor Schottky barrier for the PZ ZnO NW
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Microsystems LaboratoryUC-Berkeley, ME Dept.
Electromechanically
coupled discharging
process of aligned
piezoelectric ZnO
NWs observed in
contact mode.
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Microsystems LaboratoryUC-Berkeley, ME Dept.
Piezoelectricity of Monolayer MoS2
W. Wu, et al, Nature 2014, 514, 470.15
Second-Harmonic Generation(SHG)
Microsystems LaboratoryUC-Berkeley, ME Dept.
01/30 Tuesday 1pm: Harrison Khoo, Ian Connett,Martin Xu
01/30 Tuesday 2pm: Dan Xu, Vedang Patankar
01/30 Tuesday 4pm: Margann Rui, Tiffany, Vatsal
01/31 Wensday 3pm: Amruth,Marina Rizk, Lujain Alobaide, Nate
02/01 Thursday 1pm: Neil, Junpyo Kwon
Lab Experiment ScheduleEtcheverry Hall 1113
Microsystems LaboratoryUC-Berkeley, ME Dept.
Flexible Electrostatic TransducerPart II:
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Microsystems LaboratoryUC-Berkeley, ME Dept.
An electret is a piece of dielectric material exhibiting a quasi‐permanent electric charge
Electrets
J. A. Malecki, PRB 1999, 59, 9954
Even hundreds of years
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Microsystems LaboratoryUC-Berkeley, ME Dept.Corona Discharge
[ C C ]
F F
F F
n
Corona charge
A
-15 kV
Electret
Needle
Electrode
Electret material: Teflon (PTFE)
Charges injection
G. M. Sessler, Electrets(2nd ed), Berlin: Springer‐Verlag, 198719
Microsystems LaboratoryUC-Berkeley, ME Dept.
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Surface Potential Detection
0 5 10 15 20 25 300
-1
-2
-3
Surf
ace
Pote
ntia
l (kV
)
Time (Day)
PE
0 5 10 15 20 25 300
-1
-2
-3
-4
Surf
ace
Pote
ntia
l (kV
)
Time (Day)
pp
PP
0 5 10 15 20 25 300
-2
-4
-6
-8Su
rfac
e Po
tent
ial (
kV)
Time (Day)
PTFE
0 5 10 15 20 25 300
-2
-4
Surf
ace
Pote
ntia
l (kV
)
Time (Day)
PET
0.1-1 mC/m2
Microsystems LaboratoryUC-Berkeley, ME Dept.Example: Paper-Based
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Paper Metal (M) Polymer
Paper
Coating P@Pre-Paper
Assembling
Ⅱ Ⅲ ⅣⅠ
100 μm 500 nm
Evaporate M
Q. Zhong & J. Zhong et al., Energy Environ. Sci., 2013, 6, 1779
Charge Injection
PTFE
Microsystems LaboratoryUC-Berkeley, ME Dept.
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Example: Cloth-Based Shirt
S. Li, Q. et al, ACS Applied Materials & Interfaces 2015, 7, 14912.
Microsystems LaboratoryUC-Berkeley, ME Dept.
Challenges
Microsystems LaboratoryUC-Berkeley, ME Dept.
0.0 0.1 0.2-6
-3
0
3
Cur
rent
(A)
Time (s)0 2 4
0
1
2 Experimental Fitting
Forc
e (N
)
Lateral Distance (mm)
SampleMeter
/2 2 6
03.46 10
T
eW I Rdt J
/2 3
01.07 10
A
FW Fds J
100% 0.32%e
F
WW
Efficiency:
Input mechanical energy:
Output electricity:
I: Energy Conversion Efficiency
Measurement system
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Microsystems LaboratoryUC-Berkeley, ME Dept.
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II: Output Power
Larger Power, More Applications!
Improving the Charge Density of the Electret and the Device Structure!
Wang, Z. L.; Angew. Chem. Int. Edit. 2012, 51, 11700.
Microsystems LaboratoryUC-Berkeley, ME Dept.
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BOPP PET
PTFEPI PE
PDMS
FEP
0
-2
-4
-6
-8
Surf
ace
Pote
ntia
l (kV
)
Original Recovering
III: Package (against water)
Electret Film against Harsh Environment is a challenge!
Microsystems LaboratoryUC-Berkeley, ME Dept.
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Microsystems LaboratoryUC-Berkeley, ME Dept.Summary
Three Typical Application FieldsAssistance of Internet of Things
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WearableElectronics
Self-poweredSensors
Energy Harvesting
W. Li and J. Zhong et al, Adv. Funct. Mater., 2015, 26,1964
Microsystems LaboratoryUC-Berkeley, ME Dept.
Intro to MicroRobots
Microsystems LaboratoryUC-Berkeley, ME Dept.
30Liwei Lin, University of California at Berkeley
Microsystems LaboratoryUC-Berkeley, ME Dept.
Flying Insects
Artificial Flying Insects
Category
Nano Hummingbird Robotic Insect Microrobot
Size 15cm 3cm 1.5cm
Status Autonomous flight Tethered flight Flapping motion
Actuator DC motor PZT ElectrostaticM. Karpelson, G. Y. Wei, R. J. Wood, "A review of actuation and power electronics options for flapping-wing robotic insects,"
2008 Ieee International Conference on Robotics and Automation, Vols 1-9, pp. 779-786, 2008.
Microsystems LaboratoryUC-Berkeley, ME Dept.
Actuators
Actuators for Artificial Flying Insects
M. Karpelson, G. Y. Wei, R. J. Wood, "A review of actuation and power electronics options for flapping-wing robotic insects," 2008 Ieee International Conference on Robotics and Automation, Vols 1-9, pp. 779-786, 2008.
Actuator
DC motor PZT Electrostatic
AdvantageHigh drive efficiencyDC power electronics
Linear motionHigh power density
High drive efficiencyMiniaturization (easy)
DisadvantageRotary motion
Miniaturization (hard)AC power electronics
Low efficiencyPull-in effectLow lift force
Vibration Forced Vibration (Flapping Frequency =Input Signal )
Microsystems LaboratoryUC-Berkeley, ME Dept.
Inspiration from Nature
Insects Muscle’s Vibration
Flapping signal ≠ Neural signal Self-excited vibration
R. Josephson, J. Malamud, D. Stokes, "Asynchronous muscle: a primer," J. Exp. Biol., vol. 203, pp. 2713-2722, 2000.
Microsystems LaboratoryUC-Berkeley, ME Dept.
Research Concept and Approach
Electrostatic Actuation
Electrostatic actuator Our actuator
Advantages
Linear motionMaintain
the advantages by using electrostatic actuation.
High drive efficiency
Ease of miniaturization
Disadvantages
Pull-in effectOvercome
the disadvantages by using self-excited vibration.
AC power electronics
Low lift force
Microsystems LaboratoryUC-Berkeley, ME Dept.
Self-excitation
Self-excited Vibration of Beam
Experimental setup Insulated base Metal beam DC power sourceVibration course Electrostatic induction No Pull-in effect Charging and discharging
Xiaojun Yan, Mingjing Qi, Liwei Lin, An autonomous impact resonator with metal beam between a pair of parallel-plate electrodes, Sensors & Actuators: A. Physical , pp. 366-371, 2013.
Microsystems LaboratoryUC-Berkeley, ME Dept.
Operating Principle
Vibration Course of the Beam (top view)
Xiaojun Yan, Mingjing Qi, Liwei Lin, An autonomous impact resonator with metal beam between a pair of parallel-plate electrodes, Sensors & Actuators: A. Physical , pp. 366-371, 2013.
Structure parameters Materials: gold bonding wire Length: 10.5mm Diameter: 25.4μm DC voltage: 1100VVibration parameters Amplitude: 4.5mm Frequency: 80Hz
Microsystems LaboratoryUC-Berkeley, ME Dept.
Actuator Design
Configuration
Flapping wing assembly: Four parallel beams and two wings Parallel metal beams: Enhance the driving force Two wings: Extracted from honey bees Fulcrum bars with oval holes: Allow the beams to rotate
Microsystems LaboratoryUC-Berkeley, ME Dept.Flipping & Rotation
Rotational Fulcrum Bars
Electrostatic induction Incline to electrodes Contact and charged Reverse direction Flap and rotation
Microsystems LaboratoryUC-Berkeley, ME Dept.
Experimental Setup
Experimental Tests
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Experimental Setup
Lift Force
Microsystems LaboratoryUC-Berkeley, ME Dept.
Comparisons with Insects
Flapping Motion
Realinsect
Ouractuator
Microsystems LaboratoryUC-Berkeley, ME Dept.
Video Demo
Flapping Motion
Microsystems LaboratoryUC-Berkeley, ME Dept.
Experimental Results
Operation Frequency Characterizations
Decrease with gap distance d0
Microsystems LaboratoryUC-Berkeley, ME Dept.
Effects of Electrode Gap Distance
Flapping Angle Characterizations
Increase with d0 under high voltage Decrease with d0 under low voltage
Microsystems LaboratoryUC-Berkeley, ME Dept.
FLift
Lift Force vs Gap Distance
Lift Force Characterizations
Increase with d0 under high voltage Decrease with d0 under low voltage
Microsystems LaboratoryUC-Berkeley, ME Dept.
Vertical Lift-Off Setup
Vertical Takeoff
U-shape rail: Allow the assembly to move upward Extended electrodes: Provide continuous driving force
Upward speed: 2.2mm/s Frequency: 70Hz
Microsystems LaboratoryUC-Berkeley, ME Dept.
Visual Demonstration of Lift Force
Video Demo
Microsystems LaboratoryUC-Berkeley, ME Dept.
Design to Enhance Wing Rotation
Structure Optimization
One oval hole Two holes setup
Microsystems LaboratoryUC-Berkeley, ME Dept.
Video Demo
Enhanced Rotational Motion
Microsystems LaboratoryUC-Berkeley, ME Dept.
Conclusion
The actuator can be excited into resonance with frequency of 50-70Hz by simply DC power source.
The actuator can drive two insect wings into reciprocation with flapping amplitude up to 48.5.
The flapping wing assembly can generate effective lift force (up to 3.1mg) high enough to result in self-lifting.
Our next work aims at further enhancing the lift force and reducing the total weight, for the purpose of realizing the takeoff of the whole actuator.