27892069 a MEMS Based Piezoelectric Power Generator Array for Vibration Energy Harvesting
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Transcript of 27892069 a MEMS Based Piezoelectric Power Generator Array for Vibration Energy Harvesting
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Microelectronics Journal 39 (2008) 802806
A MEMS-based piezoelectric power generator array for vibration
energy harvesting
Jing-Quan Liua,, Hua-Bin Fanga, Zheng-Yi Xub, Xin-Hui Maob, Xiu-Cheng Shena,Di Chena, Hang Liaob, Bing-Chu Caia
aNational Key Lab of Micro/Nano Fabrication Technology, Key Lab for Thin Film and Micro-fabrication Technology of Ministry of Education,
Institute of Micro/Nano Science and Technology, Shanghai Jiao Tong University, Shanghai 200030, PR ChinabACS Sensors Lab, Honeywell, Shanghai 201203, PR China
Received 13 September 2007; accepted 15 December 2007
Available online 20 February 2008
Abstract
Piezoelectric power generator made by microelectromechanical system (MEMS) technology can scavenge power from low-level
ambient vibration sources. The developed MEMS power generators are featured with fixed/narrow operation frequency and power
output in microwatt level, whereas, the frequency of ambient vibration is floating in some range, and power output is insufficient. In this
paper, a power generator array based on thick-film piezoelectric cantilevers is investigated to improve frequency flexibility and power
output. Piezoelectric cantilevers array has been designed and fabricated. The cantilevers array can be tuned to the frequency and
expanded the excited frequency bandwidth in ambient low frequency vibration. Serial connection among cantilevers of the array is
investigated. The prototype generator has a measured performance of 3.98mW effective electrical power and 3.93 DC output voltage to
resistance load. This device is promising to support networks of ultra-low-power, peer-to-peer, wireless nodes.
r 2007 Elsevier Ltd. All rights reserved.
PACS: 84.60.Bk; 85.85.+j; 85.50.n
Keywords: Energy harvesting; MEMS; Cantilevers array; Vibration frequency; Serial connection; Low frequency
1. Introduction
With the recent advances in wireless and microelec-
tromechanical system (MEMS) technology, sensors have
the ability to be placed almost anywhere [1,2]. Due to the
nature of these wireless sensors, it is urgent that they
contain their own power supply. In most cases this power
supply is the conventional battery. However, the batteryhas a finite lifespan and once extinguished of its power, the
sensor must be retrieved and the battery replaced. With
these sensors being placed in remote location it can become
an expensive task to obtain and replace the battery.
Energy harvesting from ambient vibration by MEMS
technology is one of the promising alternatives. The
vibration can be converted to electric energy using three
types of electromechanical transducers: electromagnetic [1],
electrostatic [1], and piezoelectric [216]. Piezoelectric
vibration-to-electricity converters have high electromecha-
nical coupling, require no external voltage source and are
particularly attractive for use in MEMS especially for
volume-limited wireless sensor node [11]. Glynne-Jones
et al. [9,10] and Shu and Lein [11] provided an approach to
design, model and optimize the conversion efficiency of thevibration generator. Jeon developed a thin film piezo-
electric power generator based on MEMS using a d33
mode. Its resonant operation frequency is at 13.7 kHz [12].
Roundy reported a kind of prototype of tiny, piezoelectric
cantilever (925 mm in length) with a relatively heavy mass
on the free end, which can generate 375 mW from a
vibration source of 2.5 m/s2 at 120Hz. The scale of the
device, however, is larger than that of most MEMS devices
[13]. duToit et al. [14] proposed a prototype for low-
level ambient MEMS harvester. Another MEMS-based
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www.elsevier.com/locate/mejo
0026-2692/$ - see front matterr 2007 Elsevier Ltd. All rights reserved.
doi:10.1016/j.mejo.2007.12.017
Corresponding author.
E-mail address: [email protected] (J.-Q. Liu).
http://www.elsevier.com/locate/mejohttp://dx.doi.org/10.1016/j.mejo.2007.12.017mailto:[email protected]:[email protected]://dx.doi.org/10.1016/j.mejo.2007.12.017http://www.elsevier.com/locate/mejo -
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piezoelectric power generator designed to harvest low
frequency vibration energy by adding nickel proof mass
based on UV-LIGA technology [15,16].
So far, the developed MEMS power generators are
featured with fixed or narrow operation frequency and
power output in microwatt level, whereas the frequency of
ambient vibration is floating in some range, and microwattis insufficient to power current sensing node. In this paper,
a power generator array based on thick-film piezoelectric
cantilevers is investigated to improve power output and
frequency flexibility. Also, since many sources in the
ambient vibration are in the low frequency (o1000 Hz),
the cantilevers are designed working under low frequency
range.
2. Structure design and prototype fabrication
Cantilever beam configuration is chosen for its simpli-
city, compatibility with MEMS manufacturing processes,
and its low structural stiffness. The beam configuration is a
structure consisting of a silicon base frame, a single
piezoelectric element (layer sandwiched between a pair ofmetal (Pt/Ti) electrodes), and a proof metal mass in free
end, as illustrated in Fig. 1.
The cantilever device operates as follows. When base
frame of the device is vibrated by environmental ground-
work, simultaneous input force feeds into this second-order
mechanical system, then some parts of the cantilever will
move relatively to the base frame. That relative displace-
ment causes the piezoelectric material in the system to be
tensed or compressed, which in turn induces charge shift
and accumulation due to piezoelectric effect. Magnitude of
the electric charge voltage is proportional to the stress
induced by the relative displacement.
It is well known that resonant vibration can amplify the
relative displacement remarkably. Thus, the micro gen-
erators mechanically resonate at a frequency of the
ambient vibration can generate maximum electrical power.
Natural frequency of structure is approximately given as
$ ffiffiffiffiffiffiffiffiffik=m
pby its stiffness (k) and mass (m). This indicates
that varying structure dimension of the cantilever can
regulate the natural frequency of the power generator.
A single cantilever power generator device [10] reveals the
performance of its output voltage under different excited
frequency in Fig. 2. It shows that the output voltage drops
off dramatically when the excited frequency deviates from
resonant point. To locate in range of X1=ffiffiffi2p maximum
output voltage, the available bandwidth is just within
723 Hz. The narrow available bandwidth of the device
extremely restricts its practical application in ambient
vibration.
Under many circumstances, the driving frequency will be
known before the device is designed and fabricated. In
other situations, however, this frequency will not be known
a prior, or it may change over time. It is also relevant to
consider the mass fabrication of such devices. So it would
clearly be advantageous to create a device that can operate
effectively over a range of vibration frequencies.
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Fig. 1. Schematic configuration of single cantilever beam.
Fig. 2. Output voltage as a function of excited frequency.
Fig. 3. Fabrication process of micro power generator array: (1) functional films preparation: SiO2/Ti/Pt/PZT/Ti/Pt, (2) functional films pattern, (3) silicon
slot etching by RIE, (4) back silicon deep etching by KOH solution, (5) cantilever release by RIE, and (6) metal mass micro fabrication and assemblage.
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Roundy et al. [13] developed two solutions to tune
resonance frequency of beam. One is to apply an axial
preload by set-screws or other devices that push on the
clamps at either end of the beam, which passively control
the stiffness (k) of the beam to tune its resonance point.
The second active tuning method is to design device with a
wider bandwidth that connects N springmassdampersystems in one long cantilever.
The two solutions are effective to address resonance
frequency issue, but they are not available in MEMS
fabrication due to its relative complicated structure.
The overlapping effect of resonance frequency is
introduced in our design. A MEMS array with multi-
cantilevers is designed with its single cantilever behaving
closer resonance frequency one after another. Each
cantilever is one springmassdamper system with one
degree of freedom. When cantilevers with closer resonance
frequency connected together as an array, the available
bandwidth will cover the range of minimum to maximum
resonance value of the cantilevers in the array. On the other
hand, MEMS fabrication technology ensures the advan-
tage of mass production of cantilevers with various
structure parameters in an array.The techniques of micro fabrication used here mainly
involve functional films preparation and pattern, bulk
silicon micromachining, structure release and mass assem-
blage [15,16]. Firstly, cantilevers with closer resonance
frequency are designed with proper structure parameter.
The center level of resonance frequency is determined by
the target vibration frequency level. And the structure
parameters can be selected through mature modal simula-
tion such as using ANSYS software. Based on the design
for structure parameters selection and cantilevers distribu-
tion in array, mask layout for MEMS fabrication can be
prepared. The detail of fabrication process can refer in
Ref. [16,17]. Although Ref. [15,16] only introduces one
single cantilever, the process of cantilevers-array is similar
with Ref. [15,16]. Fig. 3 illustrates the fabrication process.
A made-up power generator array is shown in Fig. 4. The
size of the cantilevers is of 12 mm silicon layer thickness,
3.2 mm PZT layer thickness, the length and width are in
range of 20003500 and 7501000 mm respectively. And the
natural frequency is in 200400 Hz range.
3. Testing and analysis
The vibration-electricity measurement is executed with
the fabricated power generator standing in a controllablevibration source (the vibration frequency is adjustable and
the vibration acceleration is 0.5 g). The metal pads on top
and bottom electrodes are connected to the load (resistor)
through the down-lead, using oscilloscope to monitor and
record the load voltage signal. Fig. 5 shows the schematic
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Fig. 4. Picture of power generator array prototype.
Fig. 5. Performance testing of piezoelectric power generator: (1) natural frequency and AC output voltage, (2) AC power output delivered to adjustable
resistor, (3) voltage after bridge rectification (4) capacitor charge.
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configuration of testing methods and measurements for
each single cantilever.
Three cantilevers (C1, C2, and C3) as an array are taken
as measurement sample in the testing and analysis. Therelated information is listed in Table 1. The bandwidth
covers from 226234 Hz, which indicates the cantilevers
array has wider bandwidth than that of single cantilever.
The respective performances are measured, including
natural frequency, output voltage, rectification property
and capacitor charge. Fig. 6 illustrates the performance of
cantilever C1.
As an array, these three cantilevers are electrically
connected. When they are connected directly, the AC
electrical power from different cantilevers can be counter-
acted as they have different phases. Fig. 7 shows the array
excited under frequency of 229 Hz, and the AC output
voltages of each cantilever are 2.01 V (C1), 1.64 V (C2) and
1.606 V (C3), respectively. The AC output voltage after
direct serial connection is about 3.06 V, which is far less
than the value of 2.01+1.64+1.606 5.256 V. As shownin Fig. 7, there exists phase difference of nearly 1201
between C2 and C1. The phase difference impairs the
electrical accumulation of three cantilevers. And the DC
voltage across capacitor after rectification is only 2.51 V,
and the maximum DC power output is about 3.15 mW.
One approach to this problem is provided by the
following. One DC output voltage can be attained by
rectifying an AC output voltage from each cantilever, and
DC output voltage terminals are connected in series to
achieve a higher voltage, just like serial connection of the
batteries. The output voltage from different cantilevers
cannot be counteracted. Fig. 8 shows the serial connection
method.
After ACDC rectification and serial connection of all
cantilevers together, the DC voltage goes up to 3.93 V and
the maximum DC power output is about 3.98mW.
Although the rectification circuit consumes some electrical
energy, it still takes advantage compared with the direct
connection under AC signal.
On the other hand, the cantilevers in the array connected
after ACDC rectification show wider bandwidth than that
of single one. It seems that the overlapping/accumulation
effect is effective to expand bandwidth of power generator.
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Fig. 6. Performance of one single cantilever power generator: (1) AC
output voltage on oscillograph, (2) output voltage after full wave
rectification, (3) voltage on a charging capacitor.
Fig. 7. AC output of three cantilevers in an array and their direct serial
connection.
Fig. 8. Electrical connection after ACDC rectification.
Table 1
Respective performance of the three cantilevers in the array
Cantilever
no.
Cantilever geometry (mmmm)
(different Ni mass)
Natural
frequency (Hz)
AC output
voltage (V)
DC voltage across
capacitor (V)
Maximum power
output (mW)
C1 Length3000mm; width1000mm 229 2.01 1.57 2.55
C2 234 1.86 1.43 2.1
C3 226 1.75 1.22 1.87
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4. Conclusion
In summary, a micro-power generator array has been
investigated by utilizing PZT film as the transducer to
harvest ambient low-level vibration. It is fabricated
successfully by the MEMS process. The prototype gen-
erator has a measured performance of 3.98 mW of effectiveelectrical power and 3.93 DC output voltage. The
experimental results show that the arrayed device is
promising in improving operation bandwidth and power
output of power generator. It is indicated that a potential
in the development of the power generator meets applica-
tions in wireless/embedded sensor networks.
Acknowledgements
This work is supported by Honeywell Company. The
authors also would like to thank Professor Jinrong Cheng
of Shanghai University for PZT film material preparation.
References
[1] A. Chandrakasan, R. Amirtharajah, J. Goodman, W. Rabiner,
Trends in low power digital signal processing, Int. Symp. Circuits
Syst. 4 (1998) 604607.
[2] S.P. Beeby, M.J. Tudor, N.M. White, Energy harvesting vibration
sources for microsystems applications, Meas. Sci. Technol. 17 (2006)
175195.
[3] W.J. Li, T.C.H. Ho, G.M.H. Chan, P.H.W. Leong, H.Y. Wong,
Infrared signal transmission by a laser-micromachined vibrationin-
duced power generator, in: Proceedings of the 43rd IEEE Midwest
Symposium on Circuits and Systems, vol. 1, 2000, pp. 236239.
[4] C.B. Williams, R.B. Yates, Analysis of a micro-electric generator formicrosystems, Sensors Actuators A 52 (1996) 811.
[5] R. Amirtharajah, A.P. Chandrakasan, Self-powered signal processing
using vibration-based power generation, IEEE J. Solid State Circuits
33 (1998) 687695.
[6] S. Meninger, J.O. Mur-Miranda, R. Amirtharajah, A.P. Chandra-
kasan, J.H. Lang, Vibration-to-electric energy conversion, IEEE
Trans. Very Large Scale Integr. VLSI Syst. 9 (1) (2001) 6476.
[7] R. Tashiro, N. Kabei, K. Katayama, Y. Ishizuka, F. Tsuboi,
K. Tsuchiya, Development of an electrostatic generator thatharnasses the motion of a living body, JSME Int. J. Ser. C 43 (4)
(2000) 916922.
[8] S. Roundy, P.K. Wright, J. Rabaey, A study of low-level vibrations
as a power source for wireless sensor nodes, Comput. Commun. 26
(2003) 11311144.
[9] P. Glynne-Jones, S.P. Beeby, E.P. James, N.M. White, The modeling
of a piezoelectric vibration powered generator for microsystems, in:
Proceedings of the 11th International Conference on Solid-State
Sensors and Actuators, Transducers 2001 and Eurosensors XV,
Munich, Germany, 2001, pp. 4649.
[10] P. Glynne-Jones, et al., Towards a piezoelectric vibration powered
microgenerator, IEE Sci. Meas. Technol. 148 (2) (2001) 6872.
[11] Y.C. Shu, I.C. Lien, Efficiency of energy conversion for a piezo-
electric power harvesting systems, J. Micromech. Microeng. 16 (2006)
24292438.[12] Y.B. Jeon, R. Sood, J.H. Jeong, S.G. Kim, MEMS power generator
with transverse mode thin film PZT, Sensors Actuators A 122 (2005)
1622.
[13] S. Roundy, E.S. Leland, J. Baker, E. Carleton, E. Reilly, E. Lai,
B. Otis, J.M. Rabaey, P.K. Wright, V. Sundararajan, Improving
power output for vibration-based energy scavengers, IEEE Pervasive
Comput. 4 (2005) 2836.
[14] N.E. duToit, B.L. Wardle, S.G. Kim, Design considerations for
MEMS-scale piezoelectric mechanical vibration energy harvesters,
Integr. Ferroelectr. 71 (2005) 121160.
[15] H.B. Fang, J.Q. Liu, Z.Y. Xu, D. Chen, B.C. Cai, A MEMS-based
piezoelectric power generator for low frequency vibration energy
harvesting, Chinese Phys. lett. 23 (2006) 732734.
[16] H.B. Fang, J.Q. Liu, Z.Y. Xu, D. Chen, B.C. Cai, Fabrication and
performance of a MEMS-based piezoelectric power generator forvibration energy harvesting, Microelectron. J. 37 (2006) 12801284.
ARTICLE IN PRESS
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