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

    ARTICLE IN PRESS

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    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.

    J.-Q. Liu et al. / Microelectronics Journal 39 (2008) 802806 803

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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.

    ARTICLE IN PRESS

    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.

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