New Energy Technology Forum(13:00 ~ 14:45, Monday 23rd April)
New Energy Technology Forum(13:00 ~ 13:15, Monday 23rd April)
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New Energy Technology Forum(13:15 ~ 13:30, Monday 23rd April)
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New Energy Technology Forum(13:30 ~ 13:45, Monday 23rd April)
1aOA03
New Energy Technology Forum(13:45 ~ 14:00, Monday 23rd April)
1aOA04
Three-dimensional ceramic molding
based on microstereolithography for the production
of piezoelectric micro power generation devices
Kensaku Monri and Shoji Maruo
Yokohama National University
79-5 Tokiwadai, Hodogaya, Yokohama, Kanagawa, Japan
email:[email protected]
Maruo laboratory , Yokohama National University
Research background Wireless Sensor Networks
Networks to collect information ubiquitously using wireless sensor nodes
PC
Various types of wireless sensor nodes are required.
industrial process monitoring and control, machine, health monitoring, etc. Industrial and consumer applications
Large size High power
Small size Low power
wireless sensor node
Maruo laboratory , Yokohama National University
The wireless sensor nodes are often powered by conversional batteries
Battery Problems of Wireless Devices
The need either to replace or to recharge them periodically
Challenges
・Cost of battery replacement is high ・In some situations, the battery replacement is not possible
Energy harvesting is the promising alternative of the batteries Converting environment sources of energies into electrical energy
The size and weight of the batteries are relatively large
Thermal energy Light energy Wind energy
Vibrational energy is lightly affected by environmental changes.
Vibrational energy is suitable for energy harvesting devices
Vibrational energy
Maruo laboratory , Yokohama National University
maruo lab , Yokohama National University
Piezoelectric Energy Harvesting
IEEE Pervasive Compt. 4 (1) (2005) 28
Microelectronics Journal 37 (2006) 1280
Vibration is limited to one or two directions
due to the 2-D shapes of piezoelectric elements.
Length : 9-25mm
Power : 375μW(120Hz) Length×Width : 2.0×0.6mm
Power : 2.16μW(609Hz)
Height : ~1μm Diameter : ~40nm
Science 312 (2006) , 242
Power : 0.5pW(10MHz)
Previous micro/nano devices for piezoelectric energy harveting
Development of 3-D piezoelectric elements
for high-performance energy harvesting devices
Maruo laboratory , Yokohama National University
maruo lab , Yokohama National University
Microstereolithography
Single-photon stereolithography Two-photon stereolithography
Multi-scale fabrication of arbitrarily 3-D polymer molds
fs pulsed laser beam
two-photon absorption
Photopolymer
objective lens
UV laser beam
stage
0.5mm 1mm
XY Plane:20-100μm Depth(Z):50-200μm
Resolution XY Plane:100-500nm Depth(Z):500nm
Resolution
XY Plane:20×20mm Depth(Z):No limitation
Size XY Plane:300×300μm Depth(Z): ~ 200μm
Size
5mm
Lasers & Photo. Rev. 2, 100 (2008).
Opt. Lett. 22, 132 (1997) Times Cited:668
Maruo laboratory , Yokohama National University
maruo lab , Yokohama National University
3-D ceramic molding based on microstereolithography
Drying Thermal Decomposition Sintering Immersing
Polymer model Slurry
Gas
(~600℃) (~1400℃)
•Sophisticated 3-D ceramic microstructures (µm~mm scale)
•Wide variety of ceramics (Optoceramics, Bioceramics, Piezoceramics)
Jpn. J. Appl. Phys. 48, 06FK01 (2009)
1mm
SiO2 (3D channel)
Jpn. J. Appl. Phys. 50, 06GL15 (2011)
1mm
β-TCP (porous body)
10mm MNC 2010
SiO2 (Microchannel)
Microstereolithography + Floc casting of ceramics slurry
Maruo laboratory , Yokohama National University
maruo lab , Yokohama National University
Fabrication of a spiral piezoelectric element
1mm
Fabrication of a polymer mold for making a herically-curved piezoceramic element by single-photon microstereolithography
CAD image of the device ・3-D deformation
Spiral structure like a coil spring
・Increase of deformation amount
The shell structure allows insertion of slurry by centrifugal casting
Shell thickness : 100-200μm
Inlet diameter : 200μm
Maruo laboratory , Yokohama National University
・Increase of energy density of generation device
maruo lab , Yokohama National University
Ceramic Slurry
Ceramics Slurry A concentrated ceramic particulate suspension
(A mixture of ceramics powder, dispersant and ion exchange water)
BaTiO3 ceramics powder
The role of dispersant
Dispersant suppresses the aggregation of particles
High strength of a green body
High-concentration slurry
・Particle diameter : 150nm or 400nm
・Environmentally friendly material
1μm 1μm
Dispersant binds ceramic particles
KCM Corporation : BT-HP
Maruo laboratory , Yokohama National University
In preparation of slurry
In dry process
maruo lab , Yokohama National University
Thermal Decomposition Process
Precise control of heating profile is required
to reduce the collapse of the green body
Rapid thermal decomposition places great stress on a green body
Collapse of the green body
0
10
20
30
40
50
60
70
80
90
1000
50
100
150
200
250
300
350
400
450
500
550
600
0 200 400 600 800 1000 1200 1400 1600 1800 2000
Wig
ht l
oss
rate
(f)
[wt%
]
Tem
per
atu
re[℃
]
Time[min]
Temperature
Weight loss rate1mm
1mm
Maruo laboratory , Yokohama National University
maruo lab , Yokohama National University
Time [min.]
Wei
ght
loss
rat
e (f
) [
wt%
]
Tem
per
atu
re
[ ℃]
0%
10%
20%
30%
40%
50%
60%
70%
80%
90%
100%0
50
100
150
200
250
300
350
400
450
500
0 500 1000 1500 2000
theoretical value measured value heating program
Master Decomposition Curve
(MDC) theory
Optimization of heating profile by MDC theory
Jpn. J. Appl. Phys. 48 (2009) 06FK01
Nonlinear heating profile derived from MDC theory
realized constant weight loss of a polymer mold (0.05wt%/min)
dt
RT
Qexpdf
f1mk
1 t
0n1n
00
f
f0
:f Weight loss rate
:Q Activation energy
:n Reaction order
:R Gas constant
:T Temperature
:n Reaction order
:0k Arrhenius pre-exponential constant
J. Am. Ceram. Soc. 88, 2722 (2005)
Maruo laboratory , Yokohama National University
:0m Initial mass of the sample
maruo lab , Yokohama National University
Experimental Results
Green body
Sintering body
sintering temperature : 1300℃
1mm
1mm
after thermal decomposition process derived by MDC theory
Attachment of silver electrodes and
Poling treatment under electric field of 1.5 kV/mm
1mm
Maruo laboratory , Yokohama National University
maruo lab , Yokohama National University
Demonstration of Piezoelectric Property
Piezoelectric property of the spiral piezoelectric element
was confirmed by adding repetitive load.
-50
0
50
100
150
200
250
300
-150
-100
-50
0
50
100
150
0 5 10 15 20 25 30
Load
[gf]
V
olt
age[
mV
]
Time [sec.]
load cell
Maruo laboratory , Yokohama National University
maruo lab , Yokohama National University
Conclusion
Maruo laboratory , Yokohama National University
-- Making high-concentration ceramic slurry with BaTiO3 nanoparticles
-- Filling the slurry into a polymer mold at high density by centrifugal casting
-- Optimizing heating profile of thermal decomposition process by MDC theory
Demonstration of piezoelectric property of the 3-D generator
Evaluation of the performance of the 3-D micro power generator
Improvement of power generation efficiency by optimizing 3D shape
A spiral piezoelectric element was fabricated using a 3-D molding process based on microstereolithography
Future Works
New Energy Technology Forum(14:00 ~ 14:15, Monday 23rd April)
1aOA05
Energy Harvesting System Using
Ferroelectric PVDF Film
Takashi Nakajima, Soichiro Okamura Department of Applied Physics, Faculty of Science Tokyo University of Science, JAPAN
Energy Harvesting
※Quartz, PZT, AlN, ZnO, PVDF etc…
Piezo* Electrical Energy
The power sources are human, animals and automobile and so on. Clean energy
Mechanical Energy
Applications sc
ale
Technology trends
EnOcean NEC/ Soundpower
Innowattech
JR East
Pavegen
Brother Industry
MicroGen
Bridgestone
Metasphere
ETSI
Michigan Univ.
Georgia Tech
Sainsbury's supermarket
Club Watt
※Electromagnetic or piezoelectric methods
Efficiency??
• Flexible • Large area • Less environmental burden
Piezoelectric Power Generation Using Polymer
Fluorine
Hydrogen
Symmetry:C2v 3 2
1
Drawing direction
k31 d31 1/s11 e33/e0(80kHz) k33 e33 c33
0.15 15 pC/N 10 GPa 9.0 0.27 -180mC/m2 10 GPa
0 0 00 0 0𝑑31 𝑑32 𝑑33
0 𝑑24 0
𝑑15 00 00 0
PVDF
Power generating systems using polymer
Trample
•Multilayer •Large stress by lever
Vibration
•Film is very flexible •Easy to attach
PVDF
LED
Tension
•Particular usage for polymer based energy harvesting
Power generation characteristics
• Theoretical estimation • Experimental results
Estimation of power generation
pressing
drawing
vending
𝑄 = 𝑑𝐹 𝑑 coefficient: C/N
𝑉 = ℎ∆𝑙 ℎ coefficient: V/m
𝑃 =1
2
1
2𝑄
1
2𝑉 𝑓 =
1
8𝑘2𝐹∆𝑙𝑓
Under impedance matching condition,
𝑄𝑉 = 𝑑𝐹 × ℎ∆𝑙 = 𝑑2 𝜀𝑠 𝐹∆𝑙 = 𝑘2𝐹∆𝑙
load 1/2Q, 1/2V
×𝑘2/8
Mechanical Energy 𝐹∆𝑙
Estimation of power generation
𝑃 =1
8𝑘2𝐹∆𝑙𝑓
l3
l2
l1
Strain Form ⇒ when large stress can be applied
Stress Form ⇒ when available stress is limited
𝑃 =1
8𝑘2𝑐33𝑙1𝑙2𝑙3
∆𝑙3𝑙3
2
𝑓
𝑃 =1
8𝑘2𝑠11
𝑙1𝑙2𝑙3
𝐹12𝑓
Multilayer is effective.
How to deform the film? ⇒Lever structure
Smaller cross-sectional area is better →drawing is effective
Calculations of power generation
10-6
10-5
10-4
10-3
10-2
10-1
100
101
102
103
UL (
J)
10-2
10-1
100
101
Strain (%)
PZT PVDF
Break-down limit
10%
strain
=3.6J
Sample size
1cm3
The efficiency of PVDF Is smaller than PZT. However, the max power generation surpasses PZT owing to its large break down limit.
System design
Electromechanical coupling k
Output power
Frequency
Multilayer
Stress increase
Drawing
Power generating floor
Water flow
Rotational motion
Structure of energy generating system
Power generating floor Power generation from rotational motion
cam system ・Frequency upconversion
Large Stress Small Stress
50
40
30
20
10
0
UL (
J)
10 100 1000
CL (nF)
200 layers 100 layers 50 layers
Power generation characteristics of multilayer structure
10
8
6
4
2
0
Q (
C
)
1.21.00.80.60.40.20.0
F (kN)
200 layers 100 layers 50 layers
Generated Charge vs Stress Load capacitance dependence
※Stress=1 kN
Power generating floor
3.0
2.5
2.0
1.5
1.0
0.5
0.0
PL (m
W)
10 100 1000
CL (F)
50
40
30
20
10
0
UL (m
J)
25 s 20 s 15 s 10 s 5 s 1 s
Charging time
-200
-100
0
100
200
Ou
tpu
t vo
lta
ge
(V
)
20151050
t (s)
RL = 1 MΩ
Output voltage Charging characteristics
Rectification
Drawing type power generation
100
80
60
40
20
0
Q (
pC
)
1.21.00.80.60.40.20.0
Strain (%)
d31=15 pC/N
18 mm×6 mm×0.04 mmt
Power generation from rotational motion
Qp-p=0.75 C
P = 1/2Q2/Cf = 8 mW
-1.0
-0.5
0.0
0.5
1.0
Q (
C
)
100806040200
t (ms)
55 Hz
Power generation using water flow
• Irrigation water • Deep-sea • Water pipe Battery-less sensing system
Reynolds number: Re
Current velocity: U
Travelled length: d
Dynamic viscosity:
𝑅𝑒 =𝜌𝑈𝑑
𝜇
Re vortex
5 < Re < 45 Double spiral
45 < Re < 150 Karman vortex street
150 < Re Turbulent flow
Time (s)
Ou
tpu
t vo
ltag
e (V
)
80 nW
Summery
Backgrounds Applications
Energy harvesting technique using piezoelectric materials
Battery-less, wireless devices
Power generating floor Multilayered PVDF
Stress increase by a lever system
Drawing type Highly efficient
Frequency upconversion by cam
Vibrational type Easy to get energy
Water flow power generation
Piezoelectric Polymer
Robust (Output increase by lever system)
Easily formable
Various driving modes
New Energy Technology Forum(14:15 ~ 14:30, Monday 23rd April)
1aOA06
Preparation on transparent flexible piezoelectric energy harvester based on PZT
Young Ho Do, Min Gyu Kang, Hyun Cheol Song, Won Hee Lee, Chong Yun Kang, and Seok Jin Yoon
Electronic Materials Center, Korea Institute of Science and Technology, Seoul, Korea
IWPMA 201223. Apr. 20121aOA06
1.
2.
3.
4.
5.
Medical
Personal electronics
“ Piezoelectric technologies could extend to all area ”“ Piezoelectric technologies could extend to all area ”Wireless sensors
Implantable devices
Robots
Nanosensors
MEMS
Mechanical energy sources
Wind
Wave
Body movements
Driving
Piezoelectric technologies
PiezoelectricPiezoelectric
MEMS & Nanodeivces
Flexible device technologies
Bendable
Light-weight
FoldableFlexible electronics
Flexible electronics
Most polymer substrates used in flexible devices applications have a low melting temperature( 200 ~ 300 °C) Low temperature process
Transfer process
M. C. McAlpine, Nano Lett. (2010)Rogers, SMALL (2011)
Flexible device technologies
Low Temperature Heat Treatment
Low Temperature Materials
Selective Heat Treatment
T. J. Marks, Nature Mat. (2011)
AdvantageHigh temp. for the crystallization → degrade of the under-layer structuresPrior to transfer onto a selected receiver substrateReceiver substrate is not heated to high temperatures
10
0
energy (eV)
Sapphire (Transparent)
KrF Laser (248 nm, 4.99 eV)
PZT (3.2 ~ 3.6 eV)Functional layer
Receiver substrate
Sapphire
ExcimerLaser
MeltingFunctional layer
Receiver substrate
Sapphire
Lift-off
Laser lift-off (LLO) processing, or laser transfer, has recently been presented as aviable alternative to direct deposition processes for integrating dissimilar materials.
hv (laser photon energy) - Eg (Energy band gap) < 0→ Transparent to laser radiation
hv (laser photon energy) - Eg (Energy band gap) > 0→ Absorption to laser radiation
Laser Lift-Off (LLO)
Sensors device that measures a physical quantity and converts it into a signal
Energy harvesting process by which energy is captured and stored
Piezo. sensor and energy harvester
MIM structure Planar structure
Sacrificial layerStamp
Advantage• Small size• Broad frequency (dynamic) range• Light weight• 2-wire operation (IEPE)• Ultra low noise• Simple signal conditioning• Cost effective implementation
KrF Excimer Laser(Wave Length = 248 nm)
Homogenizer
Dielectric MirrorFocus Lenz
Sample
Energy Density 400~500 mJ/cm2
Laser Frequency 10 Hz
Substrate Temp. R.T.
Excimer laser lift-off system
Experimental Procedure
Target PZT
Substrate Sapphire
Base pressure High ´ 10-7 Torr
Working pressure 5 mTorr
Ar / O2 gas 28.5 / 1.5 sccm
Substrate temperature 300 ℃
rf power 100 W
Post annealingRTA, 650 ℃,
PO2 10 Torr, 10 m
P Deposition condition of PZT thin films
Experimental Procedure
Fabrication of PZT thin films
Fabrication of Flexible samples
Laser Lift-Off and Flexible devices
Deposition of sacrificial PZT layer by rf sputter
Deposition transparent electrode by dc sputter
Deposition of functional PZT layer by rf sputter
Deposition of transparent electrode by dc sputter
Polymer substrate bondingLaser radiation and sacrificial PZT melting
Sapphire substrate removal
Flexible devices based on PZT
Current and Voltage output signal
0 10 20
-2.0x10-9
0.0
2.0x10-9
-0.05
0.00
0.05
Time (s)
Vol
tage
(V)
Cur
rent
(A)
Output Voltage
Output Current
Flexible piezo. sensor & energy harvester
Flexible Piezoelectric Energy Harvesting
Current and Voltage output – reversed polarity testing
0 10 20
-2.0x10-9
0.0
2.0x10-9
-0.05
0.00
0.05
Time (s)
Vol
tage
(V)
Cur
rent
(A)
Output Voltage
Output Current
0 10 20
-2.0x10-9
0.0
2.0x10-9
-0.05
0.00
0.05
Time (s)V
olta
ge (V
)C
urre
nt (A
)
Output Voltage
Output Current
P Forward connected: negative signal, Reverse connected: positive signal→ The measured signal was generated by the flexible samples
Forward connection Reversed connection
P The piezoelectric energy harvesting properties of transparent flexiblepiezoelectric energy harvester based on PZT thin films, which werefabricated by using laser lift-off process (LLO), were investigated.
P The transparent flexible piezoelectric energy harvester based on PZTthin films generated true signal (output current and voltage), atperiodically pressing motion.
P LLO could be useful in the possibility of using the flexible electronics.
Conclusion
Thank you for your attention
New Energy Technology Forum(14:30 ~ 14:45, Monday 23rd April)
1aOA07
© M
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12 M
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Univ
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ität
Paderb
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Energy Harvesters Using Multiple Bimorphs
for Increased Power and
Enhanced Frequency Response
9th IWPMA
23rd April 2012, Hirosaki, Japan
Waleed Al-Ashtari, Tobias Hemsel,
Matthias Hunstig and Walter Sextro
© M
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12 M
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Agenda
Piezoelectric energy / power harvesting
Design challenges & solution approaches
Proposed harvester setup
Operation scenarios & results
Conclusions
2 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
© M
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12 M
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Univ
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Piezoelectric Energy / Power Harvesting
3 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
Task
Converting ambient
vibration energy into
electrical energy
Purpose
Powering arbitrary
low-power electronics
Examples
Wireless sensor networks, wearable devices,
and health monitoring sensors
© M
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Design Challenges & Solution Approaches
4 W. Al-Ashtari, , T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
Design Challenges
Maximum power is
generated at a certain
optimal frequency.
The optimal frequency
depends on harvester and
load characteristics.
Ambient vibration frequency
might be fluctuating and
does not fit the optimal
frequency.
Solution Approaches
Optimal frequency tuning
Bandwidth enhancement
0.9 0.95 1 1.05 1.1
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Normalized Excitation Frequency
No
rma
lize
d L
oa
d P
ow
er
© M
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Design Challenges & Solution Approaches
5 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
Frequency Tuning
Based on using
attraction force of
two magnets
Attraction force
changes with
separation distance d
Attraction force acts as
an additional spring
2 4 6 8 10
180
200
220
240
260
280
300
Separation Distance d (mm)
Op
tim
al F
requ
en
cy (
Hz)
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Design Challenges & Solution Approaches
6 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
[Shahruz 2006] [Xue et al. 2008]
Bandwidth Enhancement
Multiple cantilever
beams with different
length and proof
masses
Multiple multilayered
cantilever beams with
different width and
thickness
Outp
ut
Pow
er
(µW
)
| T
ip D
isp
lace
me
nt / A
pp
lied
Acce
lera
tio
n |
Frequency Frequency (Hz)
© M
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Proposed Harvester Setup
7 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
Magnet Pairs
Bimorphs
Base
Can be used for
frequency tuning
and bandwidth
enhancement
Easy to design
and insensitive to
manufacturing
tolerances
Multiple Multilayered Cantilever Beams with Magnetic Tuning
Plastic
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Proposed Harvester Setup
Electrical Connection
8 W. Al-Ashtari, M. Hunstig, T. Hemsel, W. Sextro / IWPMA 2011
Parallel Connection Serial Connection
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Operation Scenarios & Results
9 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
All bimorphs are tuned
to one fixed frequency.
Series connection
achieves higher load
bandwidth, but less
maximum power
than parallel connection.
Frequency Tuning
0 50 100 150 200
50
100
150
200
250
300
350
Load Resistance (k)
Load P
ow
er
( µ
W )
Single Bimorph
Three Bimorphs ( Parallel connection )
Three Bimorphs ( Series connection )
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200 220 240 260 280
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
Normalized Frequency ( Hz )
Norm
aliz
ed L
oad P
ow
er
( -
)
First Bimorph
Second Bimorph
Third Bimorph
Three Bimorphs
Operation Scenarios & Results
10 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
The bimorphs are tuned
to different certain
frequencies
Example Load Case:
Operating
frequency
f = 220 − 250 Hz
Load Rl = 80 kΩ
Bandwidth Enhancement
(Theory)
235 𝐻𝑧
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Operation Scenarios & Results
11 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
Bandwidth Enhancement
(Direct Series Connection )
Different characteristics of the
bimorphs lead to interference and thus
impede improved power harvesting
200 220 240 260 280
20
40
60
80
100
120
140
160
180
Frequency ( Hz)
Load P
ow
er
( µ
W )
Single Bimorph
Three Bimorphs
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Operation Scenarios & Results
12 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
Minimum load power in desired frequency
range is increased by factor 10!
Bandwidth Enhancement
(Series Connection Using Rectifiers )
200 220 240 260 280
20
40
60
80
100
120
140
160
180
200
Frequency ( Hz )
Load P
ow
er
( µ
W )
Single Bimorph ( Without Rectifier )
Single Bimorph ( With Rectifier )Three Bimorphs ( With Rectifiers )
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Conclusions
13 W. Al-Ashtari, T. Hemsel, M. Hunstig, W. Sextro / IWPMA 2012
The proposed setup using multiple magnetic tuned bimorphs
can be used for frequency tuning and bandwidth enhancement.
The setup is easy to design and insensitive to manufacturing
tolerances.
Connecting bimorphs in parallel is better for powering small loads
and connecting in series is better for large loads.
Using rectifiers allows for a significant bandwidth enhancement.
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Thank you very much
for your attention!
University of Paderborn
Mechatronics and Dynamics
Pohlweg 47-49
33098 Paderborn
Dr.-Ing. Tobias Hemsel
phone +49-5251/60-1805
fax +49-5251/60-1803