berkeley sensor · berkeley sensor & actuator center me 138/238 flexible mechanical-electrical...
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BERKELEY SENSOR &
ACTUATOR CENTER
ME 138/238
Flexible Mechanical-Electrical
Transducers for Self-Powered Systems
Dr. Junwen Zhong
Supported by Prof. Liwei Lin
2016/11-Present: Postdoctoral researcher in University of
California Berkeley, USA
2011/09-2016/06: PhD student in Huazhong University of
Science and Technology, China
2014/07-2015/10: Visiting student in Georgia Institute of
Technology, USA
2007/09-2011/06: Undergraduate students in Huazhong
University of Science and Technology, China
Research Projects
Wearable and Paper-Based Devices; Self-Powered Electronics; Electret andPiezoelectret Materials
He has published 11 Chinese patents, 1 USA patent and 29 papers, among which 10papers were published as the first or co-first author in the journals with IF>10(including 2 ESI highly citied papers and 2 cover papers). Some of this papers havebeen published in Energy & Environmental Science, Advanced Materials, ACSNano, and Advanced Functional Materials, with over 1550 citations.
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The internet of things (IoT) is the network of physical devices, vehicles, buildings and other
items—embedded with electronics, software, sensors, and network connectivity that enables
these objects to collect and exchange data. —— Wikipedia
“IoT will consist of almost 50 billion objects by
2020”.—— Dave Evans, Cisco
2020
Power Sources for Astronomical
Electronics & Sensors in IoT ? No !
Scientific American, Zhonglin Wang3
GeneratorConvert Human Energy to Electricity
Improve the Output Characteristics
EnergyManagement
Energy Storage& Application
Various applications
Self-Power System
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A self-powered sensor system and
its potential applications! Aiming at
entirely replace battery and/or extend
the life time of the
battery for sustainable operation.
Many devices made based on nanotechnology
may need micro- to milli-Watt scale power to operate.
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Mechanical Energy
Mechanical Energy
Ubiquitous & abundant in the ambient
Power & signal sources
Boar frequency & power ranges
Human Body Energy
T. Starner, IBM Syst. J. 1996, 35, 618
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Mechanical-Electrical Energy Conversion
PiezoelectricElectromagnetic
Electrostatic Induction
Flexible Transducers
G. Zhu, et al, Nat. Commum., 2014, 5, 3426
F. Feng, et al, Nano Energy, 2012, 1, 328
Z. L. Wang, et al, EES, 2015, 7, 426
J. Zhong, et al, ACS Nano, 2014, 6, 6273
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Electromagnetic
Ad:Large outputs, Mature technology
DisAd:Non-flexible, Heavy
Piezoelectric Electrostatic
Ad:Flexible, Miniaturize, wearable
DisAd:Little outputs,toxic
Ad:Flexible, Relative large outputs
DisAd:Bad stability, Abrasion
Comparison for 3 Principles
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Flexible Piezoelectric Transducer
Part I:
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Piezoelectricity
Piezoelectric Effect is the ability of certain materials to generate an electric
charge in response to applied mechanical stress.
Active Effect
Negative EffectQuartz
Electrical Dipoles
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Piezoelectric Materials
Single Crystal materials: Electrical Dipoles
are in order configuration to form piezoelectricity. Zinc Oxide
(ZnO), Quartz, Barium Titanate (BaTiO3), etc.
Polycrystal materials: Composed of many single crystal
piezoelectric particles. 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 electrical dipoles be regular
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Material Structure d33 (pC/N)
PMN-PT
PZT
PZT
BaTiO3
ZnO
Quartz
PVDF
Single crystal
Polycrystalline
Thin film
Thin film
Thin film
Thin film
Polymer film
2000 to 3000
250 to 700
60 to 130
191
5.9
2.3
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Piezoelectric Coefficients
Larger d33 coefficients, Larger outputs!12
Inorganic/Non-Flexible
Organic/Flexible
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Polyvinylidene Fluoride (PVDF)
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Piezoelectricity FTIR
High Performance Piezoelectric Devices Based on Aligned Arrays of Nanofibers of PVDF
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Arrays of highly aligned piezoelectric nanofibers of PVDF
400 μm 10 μm
Persano, L.; et al. Nature Com., 2013, 4, 1633
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Experimental and theoretical studies of responses of pressure sensors15
Experimental and theoretical studies of responses of flexural sensors16
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Direct-Write Piezoelectric PVDF Nanogenerator with High Energy Conversion Efficiency
L. Lin, et al., Nano Letters 2010, 10, 726.17
Electric output of a piezoelectric PVDF nanogenerator
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c
d
Stability and Energy Conversion Efficiency
Novel “3-D spacer” all fibre piezoelectric textiles for energy harvesting applications
N. Soin, T. H. et al, Energy & Environmental Science 2014, 7, 1670. 20
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Output Performances of 3D Piezoelectric Fabric Power Generator21
Question:
Can the Inorganic Piezoelectric Materials be Used to Fabricate
Flexible Transducers???
Yes!!!!With the Help of Micro-Nano Technology!!!!
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Piezoelectric Nanogenerators Based on Zinc Oxide Nanowire Arrays
Z. L. Wang, J. Song, Science 2006, 312, 242. 23
Transport is governed by a metal-
semiconductor Schottky barrier for
the PZ ZnO NW
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Electromechanically coupled
discharging process of
aligned piezoelectric ZnO
NWs observed in contact
mode.
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Power Generation with Laterally Packaged Piezoelectric Fine Wires
R. Yang, Y. Qin, L. Dai, Z. L. Wang, Nat Nano 2009, 4, 34.
Design of a piezoelectric fine wire (PFW)
generator on a flexible substrate
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Electrical output of a single-wire generator (SWG)
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Connecting two single-wire generators (SWGs) in series.
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Air/Liquid-Pressure and Heartbeat-Driven Flexible Fiber Nanogenerators as a Micro/Nano-Power Source or
Diagnostic Sensor
Z. Li, Z. L. Wang, Advanced Materials 2011, 23, 84. 29
Two normal good working FNGs for
a ‘linear superposition’ test of
output current densities
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Highly-Efficient, Flexible Piezoelectric PZT Thin Film Nanogenerator on Plastic Substrates
K.-I. Park, et al, Advanced Materials 2014, 26, 2514. 33
Schematics of the working
principle of flexible PZT thin
film NG
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Large-Area and Flexible Lead-Free Nanocomposite Generator Using Alkaline Niobate Particles and Metal Nanorod Filler
C. K. Jeong, et al, Advanced Functional Materials 2014, 24, 2620. 36
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Piezoelectricity of Single-Atomic-Layer MoS2 for Energy Conversion and Piezotronics
W. Wu, et al, Nature 2014, 514, 470.
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Second-Harmonic Generation(SHG)
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Direct-current electrical characterizations of single-layer and
bilayer MoS2 devices under strains. 41
Piezoelectric outputs from single-layer and multi-layer MoS2 devices.
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Reliable Piezoelectricity in Bilayer WSe2 for Piezoelectric Nanogenerators
J.-H. Lee, et al, Advanced Materials, 2016,17, 1606667.
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Virus-Based Piezoelectric Energy Generation
B. Y. Lee, S.-W. Lee, Nat Nano 2012, 7, 351.
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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
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Flexible Electrostatic Transducer
Part II:
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Annoying Static Electricity
Static Electricity is Useful!!!
Van de Graaff Electrostatic Generator
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Electrostatic Induction
Electrostatic induction is a method to create or generate static electricity
in a material by bringing an electrically charged object near it. This causes
the electrical charges to be redistributed in the material, resulting in one side
having an excess of either positive (+) or negative (−) charges.
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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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Electrets
[ 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, 198757
Electrode 1
Electret
0
dd1
d0
d2
Air Gap
x
ε0
εr ε0
ε0
σ1
σ2
E1
Er
E2
U+
-
(1) According to gauss law:
(2) According to kirchhoff's second law:
Combing (1) and (2):
Surface Charge Density Detection
Electrode 2
Air Gap
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Surface Potential Detection
0 5 10 15 20 25 300
-1
-2
-3
Su
rfac
e P
ote
nti
al (
kV)
Time (Day)
PE
0 5 10 15 20 25 300
-1
-2
-3
-4
Su
rfac
e P
ote
nti
al (
kV)
Time (Day)
pp
PP
0 5 10 15 20 25 300
-2
-4
-6
-8
Su
rfac
e P
ote
nti
al (
kV)
Time (Day)
PTFE
0 5 10 15 20 25 300
-2
-4
Su
rfac
e P
ote
nti
al (
kV)
Time (Day)
PET
0.1‐1 mC/m2
‐ ‐ ‐ ‐ ‐ ‐ ‐ ‐ ‐+ + + + + + + +
+ +
A
R
‐
+d2
1
2
d1
Electrostatic Induction
12
12 dd
d
er
021 Top Electrode
+ + + +
+ +
- - - - - -A
+ + + +
+ +
- - - - - -A
Pressing+ + +
- - - - - -A
+ + +
ReleasingOriginal
Working Mechanism of Flexible Electrostatic Transducer
Bottom Electrode
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Original
Pressing Equilibrium
Releasing
Simulation Results
equivalent circuit
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Pressing
Releasing
-Q (t)
R
+
-
I+Q (t)-T
V
Q (t)
T-Q (t)
E1
E2
E+
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0 5 10
0
25
50
Pea
k po
wer
den
sity
(W
/cm
2 )
r
0 5 100
150
300
Pea
k po
wer
den
sity
(W
/cm
2 )
Rx (G)
0 100 200
0
25
50
Pea
k po
wer
den
sity
(W
/cm
2 )
d0 (m)
Dielectric Coefficient of Electret
External Loading
0 5 10
0
40
80
Pea
k po
wer
den
sity
(W
/cm
2 )
v (mm/s)
Pressing Velocity
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Thickness of Electret
Factors Affecting Outputs
Arch-Shaped Flexible Generator
Q
Q2
Q1d1
d2
E1
E2
2 m1 m
Pressing
Releasing
J. Zhong & Q. Zhong et al, Nano Energy, 2013, 2, 491 64
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Power Shoe
63 LEDs, 157.5 V
0 2 4 6
0
20
40
Cu
rren
t (
A)
Time (s)
Power Textile
IR Wireless sensor
Chinese Paten No. 201320434010.7
Output current > 6 mA
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Paper-Based Flexible Generator
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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
(c) (d)
(a) (b)
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NG
Blue LED
Turn over
Turn back
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An important first step in exploring
this power harvesting approach
at macro scale
Prof. G. K. FedderIEEE Fellow
Director of The Robotics Institute
Disney Research Pittsburg
Carnegie Mellon University
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