Research Article  Open Access
Shuwen Zhang, Bo Yan, Yajun Luo, Weikai Miao, Minglong Xu, "An Enhanced Piezoelectric Vibration Energy Harvesting System with Macro Fiber Composite", Shock and Vibration, vol. 2015, Article ID 916870, 7 pages, 2015. https://doi.org/10.1155/2015/916870
An Enhanced Piezoelectric Vibration Energy Harvesting System with Macro Fiber Composite
Abstract
Selfpower supply is a promising project in various applied conditions. Among this research area, piezoelectric materialbased energy harvesting (EH) method has been researched in recent years due to its advantages. With the limitation of energy form acceptance range of EH circuit system, a sum of energy is not accessible to be obtained. To enlarge the EH quantity from the vibration, an enhanced piezoelectric vibration EH structure with piezoelectric film is developed in this work. Piezoelectricbased energy harvesting mechanism is primarily proposed in this work. The specialdesigned electric circuit for EH from macro fiber composite (MFC) is proposed and then analyzed. When the structure vibrates in its modes of frequencies, the experiments are developed to measure the EH effect. The energy harvested from the vibrating structure is analyzed and the enhanced effect is presented. The results indicate that, with the enhanced EH structure in this work, vibration energy from structure is obtained in a larger range, and the general EH quantity is enlarged.
1. Introduction
Vibration on structures occasionally plays a negative role because of its disadvantages. As a solution, vibration control has been used to overcome the disadvantages [1, 2]. Generally, active control, containing sensing, signal processing, and actuating module [2–5], is a major vibration control method. All of the abovementioned modules in the vibration control system require electric power as necessity. In some applied conditions, power supply tends to be costly and hard to achieve [6, 7]. Hence, selfpower supply becomes an ideal solution. Recently, vibration energy harvesting technology, both acting as the function of energy harvesting (EH) and decreasing the vibration amplitude, has attracted research attention. With electromechanical EH methods like voice coil, smart materials, and other methods, energy is captured and then supplied to load such as wireless sensors and microelectromechanical systems (MEMS) [5, 8–10]. The captured electric energy is adjusted and further processed for load before use [11].
Among the various EH methods, piezoelectric energy vibration harvesting is widely studied. Compared with other methods, piezoelectric material occupies less space. Piezoelectric materials are widely used to harvest the mechanical energy for the long term and low power electric loads [12–14]. As the energy quantity requirement is as small as mW magnitude or even smaller, the piezoelectric materials are seen as ideal harvesters. Wideband energy harvesting technologies are presented to increase the energy obtaining efficiency [15–18]. With the wider acceptance range (vibration frequency and amplitude), the energy harvesting quantity is enlarged, and the EH ability is increased. Besides linear system, the nonlinear vibration based EH is analyzed and the effects of EH are also presented [11, 19–21]. Besides, wireless systems offer great flexibility, increased reliability, and reduced costs compared with a wired infrastructure. The majority of sensor nodes are reliant on battery, which will require periodical replacement, and are therefore not consistent with the concept of a permanent fully embedded system. A vibration energy harvesting based wireless power autonomous supply system with piezoelectric material is presented to solve this problem [22].
In this work, the piezoelectric material macro fiber composite (MFC) is used to harvest vibration energy. To enlarge the EH ability, an enhanced electric circuit is presented after MFC to adjust the captured AC electric energy. The experimental results indicate that with the enhanced electric circuit design the vibration energy selfsupply ratio (VESR) is increased.
The rest of the paper is organized as follows. The energy harvesting mechanism is analyzed in Section 2. The experiment procedures are presented in Section 3. The energy harvesting ability is analyzed and discussed in Section 4. The conclusion is finally given in Section 5.
2. Energy Harvesting Mechanism
The electromechanical properties of the MFCbased energy harvesting system are analyzed in this section. The electromechanical effect of EH system is firstly presented, and then the captured energy is predicted in various conditions. The enhanced electric circuit is discussed and designed to enlarge the EH range. Figure 1 is the block diagram of active vibration control system with energy harvesting system in this work, while the bold lineconnected parts are the focuses presented in this work.
2.1. Electromechanical Properties of MFCCantilever Beam Structure
The electromechanical properties on this experiment are the premise of energy harvesting in this work. A cantilever beam with MFC is presented for this experiment.
According to the elastic assumption and piezoelectric theory, the electromechanical properties of MFC are simplified aswhere is the strain, is the elastic flexibility of MFC, is the stress, is the piezoelectric strain constant, and is the electric field intensity, respectively.
The electric displacement of the MFC is simplified as
According to the definition of electric displacement, the can also be described as where is the electric charge, is the electrode area of MFC, is the voltage on MFC, and is a geometry constant of MFC, respectively.
In elastic deformation range of beam and MFC and with (1)–(3), the induced voltage is described aswhere is the realtime open circuit voltage, is an electromechanical constant of the MFCbeam coupled structure, is the capacitance of MFC, and is the applied average strain of the energy harvesting MFC attached area, respectively.
Realtime energy on MFC can be calculated aswhere is the power output in one cycle.
For power outputted from energy harvesting MFC, the frequency of vibration iswhere and are the power output from MFC and frequency of vibration, respectively.
Then the power output from MFC can be calculated as
Table 1 presents the parameters of MFC, cantilever beam, and whole vibrating structure. The first and second modes of cantilever beam without MFC attached are theoretically calculated as 8.42 Hz and 52.76 Hz. The first and second modes of MFCbeam coupled structure are measured as 8.30 Hz and 51.99 Hz with finite element method (FEM).

2.2. Enhanced Energy Harvesting Circuit Design
Energy is harvested from the vibrating beam with the initial form of AC electric power. The general schematic diagram of the enhanced EH circuit is presented in Figure 2. Realtime voltage varies as the vibration amplitude changes. A fullbridge rectifier and stabilization capacitance are employed after MFC. DC voltage from the fullbridge rectified circuit and capacitance is still not fit for use because its amplitude is not stable and not fit for the requirement as the vibration alters. Commercial DCDC converter enlarges the input DC voltage range in some way and outputs stable DC voltage with a certain value. When structure vibrates in smaller or larger scale, the induced is lower or higher than the input range of the commercial DCDC converter. Thus, a circuit with the function of adjusting DC voltage is necessary.
In Figure 2, – is the fullbridge rectifier. is the filtering capacitance. is the switching transistor, which is controlled by a modulator circuit. The control signal is from the sensing MFC beside the energy harvesting MFC. When , is on. Then power is supplied to inductance . When , is off. The current keeps on because the inductance restores energy. After one cycle, is on again. Then a new cycle starts. When the procedure is stable, it is known from inductance thatwhere is the realtime voltage on inductance ; is the cycle of modulator circuit.
According to the stable condition in one cycle, it is known that
Then the output voltage can be calculated aswhere is the average open circuit voltage of output, is the ontime of , and is the offtime of a cycle.
It is known from (10) that when is larger than , the voltage is boosted. When is smaller than , is bucked. This rate is controlled by SCM according to the sensing signals from sensing MFC. Based on the experiment reliability, is set in the range of 1/4~4 in this work.
2.3. Schematic Explanation of Enhanced Circuit Design
The enhanced EH circuit converts the electric power from abandoned forms to accessible forms. It widens the energy harvesting range with wideband frequency of vibration and larger vibration amplitude range. This circuit enlarges the energy harvesting ability.
Figure 3 presents the function of the enhanced circuit design. When DC voltage from rectifier is off from the acceptance range of DCDC converter, harvested energy is abandoned, as seen from the region above plane 1 and below plane 2 in Figure 3. With enhanced circuit design, the accessible range is enlarged. Plane 1 rises to plane 1′ and plane 2 drops to plane 2′. Then larger energy forms become accessible.
3. Experiments
In this work, experiments are primarily developed to obtain the electromechanical properties of the MFCbeam system. The enhanced EH circuit is then tested to adjust the DC voltage value from MFC.
3.1. Experiment System
The energy harvesting system is a part of the active vibration control system. Figure 4 is the active vibration control system with EH work presented in this work. Dynamic signal is generated from the signal source, which is then sent to the piezoelectric material driver. The driver outputs the driving voltage to the actuating MFC and makes the structure vibrate. The vibration amplitude and frequency are tested by the laser sensing system. The EH MFC captures the vibration energy and converts it to AC electric voltage form. The enhanced EH circuit converts the electric power form and adjusts the voltage value mentioned in Section 2.2. The control signal is from the sensing MFC.
3.2. Electromechanical Properties of EH Structure
Figure 5 reflects the electromechanical properties of the EH structure. Figure 5(a) is the relationship between the displacement on laser sensing point and the applied average strain of the EH region. It is clear from Figure 5(a) that in 0–3.2 mm, applied average strain of the EH region is proportional to the displacement of the sensing point. Figure 5(b) is the charge outputstrain curve from MFC.
(a)
(b)
3.3. Measurement of Electric Output
A realtime waveform of MFC output and displacement is given in Figure 6. Since the oscilloscope is straightly connected with EH MFC to observe the output waveform, the real open circuit voltage generated from EH MFC (seen from Figure 6) is not the same as the data measured by oscilloscope. The real voltage value is calculated according to the impedance rate of oscilloscope and EH MFC at the vibration frequency. The ratio of the measured value and the real value (at 8.3 Hz) is calculated aswhere is the measured voltage value of oscilloscope, is the impedance of oscilloscope at 8.3 Hz, and is the impedance of MFC at 8.3 Hz, respectively.
Figure 7 presents the realtime voltage output and its rectified waveform displayed on oscilloscope when the sensing vibrating amplitude is 3.2 mm.
As piezoelectric materials show capacitive property, the realtime voltage value on MFC is also calculated aswhere is the charge value on the EH MFC. To smooth the DC waveform and restore energy, a capacitance is connected behind the rectifier. μF is adopted in this experiment. DC voltage increases as approximately 2.2 V/s on capacitance as the 8.30 Hz vibrating amplitude is 3.2 mm on sensing edge.
Figure 8 is the DC waveform from the enhanced circuit design output at different conditions. The output DC voltage is able to be increased or decreased by raising or decreasing the duty ratio () of the control signal. When the vibration amplitude is lower than the floor level of DCDC converter, the enhanced circuit increases the voltage amplitude into the input available range. When voltage is higher than the upper level of DCDC converter, it decreases the DC voltage as the same way. Burrs can be smoothed by capacitance.
4. Energy Harvesting Ability Analysis
The vibration energy selfsupply ratio (VESR) is defined to describe the energy harvesting ability. In this discussion, the load value is defined as 2 mW. When harvested energy is surplus, the extra part will be restored (VESR > 1). The vibrating energy may just be sufficient for supplying the load (VESR = 1). When vibration energy harvesting quantity is not sufficient for load, VESR is necessary to explain the EH efficiency (VESR < 1).
The VESR is defined as where is VESR of EH power supply and is the power requirement of the signal processing circuit, respectively.
When the harvested energy is surplus, the extra energy is restored on EH capacitance (). When , the EH energy is just sufficient for load. The adjusted energy becomes a part of the power for load when . In this analysis, the two resonance frequencies mentioned in Section 2.1 are used to discuss the energy harvesting effect. Since surplus energy is restored in EH capacitance, the analysis just focuses on the situation of . Figure 9 reflects the energy harvesting effect when . With the enhanced circuit design, the accessible range of 8.3 Hz vibration has expanded from 167.48 με~334.95 με to 41.86 με~1339 με. The accessible range of 51.99 Hz vibration has expanded from 67.2 με~134.4 με to 16.83 με~537.6 με.
Figure 10 reflects the effect of the enhanced EH circuit in different vibration frequencies. EH ability is enlarged with the enhanced circuit design: area between the accessible upper limit and the accessible lower limit is enlarged in different vibration frequencies.
Figure 11 reflects this relationship between the power output and the impedance ratio of EH system and the load when the vibration is at 2 resonant frequencies. It is seen from Figure 11 that when the load impedance value is the same as the EH system, the energy output reaches the maximum value.
5. Conclusion
In this work, an enhanced vibration energy harvesting system with MFC is presented. The electromechanical coupling properties and function of enhanced EH circuit have been analyzed. Experiments are developed to test the electric output of the EH system. The experimental result proves that the enhanced circuit design is able to step up and step down the DC voltage in wide frequency range. This work helps harvest more vibration energy. The relationship between power and load impedance is provided for optimizing the circuit impedance as load varies. With the experimental EH method presented in this work, the piezoelectricbased energy harvesting ability is increased.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgment
This work is supported by the National Natural Science Foundation of China (Grant nos. 11172229 and 11321062).
References
 V. Mudupu, M. B. Trabia, W. Yim, and P. Weinacht, “Design and validation of a fuzzy logic controller for a smart projectile fin with a piezoelectric macrofiber composite bimorph actuator,” Smart Materials and Structures, vol. 17, no. 3, Article ID 035034, 2008. View at: Publisher Site  Google Scholar
 J. Schröck, T. Meurer, and A. Kugi, “Control of a flexible beam actuated by macrofiber composite patches: I. Modeling and feedforward trajectory control,” Smart Materials and Structures, vol. 20, no. 1, Article ID 015015, 2011. View at: Publisher Site  Google Scholar
 H. A. Sodano, G. Park, and D. J. Inman, “An investigation into the performance of macrofiber composites for sensing and structural vibration applications,” Mechanical Systems and Signal Processing, vol. 18, no. 3, pp. 683–697, 2004. View at: Publisher Site  Google Scholar
 J. Schrock, T. Meurer, and A. Kugi, “Control of a flexible beam actuated by macrofiber composite patches: II. Hysteresis and creep compensation, experimental results,” Smart Materials and Structures, vol. 20, Article ID 015016, 2011. View at: Google Scholar
 B. Yan, X. Zhang, and H. Niu, “Design and test of a novel isolator with negative resistance electromagnetic shunt damping,” Smart Materials and Structures, vol. 21, no. 3, Article ID 035003, 2012. View at: Publisher Site  Google Scholar
 H. Painter and J. Flynn, “Current and future wetmate connector technology developments for scientific E scabbed observatory application,” in Proceedings of the MTS/IEEE OCEANS, pp. 881–886, Boston, Mass, USA, September 2006. View at: Google Scholar
 T. Kojiya, F. Sato, and H. Matsuki, “Construction of noncontacting power feeding system to underwater vehicle utilizing electromagnetic induction,” in Proceedings of the Oceans 2005—Europe, vol. 12, pp. 709–712, 2005. View at: Google Scholar
 X. Zhang, H. Niu, and B. Yan, “A novel multimode negative inductance negative resistance shunted electromagnetic damping and its application on a cantilever plate,” Journal of Sound and Vibration, vol. 331, no. 10, pp. 2257–2271, 2012. View at: Publisher Site  Google Scholar
 A. Erturk and D. J. Inman, “An experimentally validated bimorph cantilever model for piezoelectric energy harvesting from base excitations,” Smart Materials and Structures, vol. 18, no. 2, Article ID 025009, 2009. View at: Publisher Site  Google Scholar
 K. A. CookChennault, N. Thambi, and A. M. Sastry, “Powering MEMS portable devices—a review of nonregenerative and regenerative power supply systems with special emphasis on piezoelectric energy harvesting systems,” Smart Materials and Structures, vol. 17, no. 4, Article ID 043001, 2008. View at: Publisher Site  Google Scholar
 M. Lallart and D. Guyomar, “An optimized selfpowered switching circuit for nonlinear energy harvesting with low voltage output,” Smart Materials and Structures, vol. 17, no. 3, Article ID 035030, 2008. View at: Publisher Site  Google Scholar
 J.Q. Liu, H.B. Fang, Z.Y. Xu et al., “A MEMSbased piezoelectric power generator array for vibration energy harvesting,” Microelectronics Journal, vol. 39, no. 5, pp. 802–806, 2008. View at: Publisher Site  Google Scholar
 D. Shen, J.H. Park, J. H. Noh et al., “Micromachined PZT cantilever based on SOI structure for low frequency vibration energy harvesting,” Sensors and Actuators, A: Physical, vol. 154, no. 1, pp. 103–108, 2009. View at: Publisher Site  Google Scholar
 H.B. Fang, J.Q. Liu, Z.Y. Xu et al., “Fabrication and performance of MEMSbased piezoelectric power generator for vibration energy harvesting,” Microelectronics Journal, vol. 37, no. 11, pp. 1280–1284, 2006. View at: Publisher Site  Google Scholar
 M. Ferrari, V. Ferrari, M. Guizzetti, B. Andò, S. Baglio, and C. Trigona, “Improved energy harvesting from wideband vibrations by nonlinear piezoelectric converters,” Procedia Chemistry, vol. 1, no. 1, pp. 1203–1206, 2009. View at: Publisher Site  Google Scholar
 F. Cottone, L. Gammaitoni, H. Vocca, M. Ferrari, and V. Ferrari, “Piezoelectric buckled beams for random vibration energy harvesting,” Smart Materials and Structures, vol. 21, no. 3, Article ID 035021, 2012. View at: Publisher Site  Google Scholar
 B. Yang, C. Lee, W. Xiang et al., “Electromagnetic energy harvesting from vibrations of multiple frequencies,” Journal of Micromechanics and Microengineering, vol. 19, no. 3, Article ID 035001, 2009. View at: Publisher Site  Google Scholar
 L. Gu and C. Livermore, “Impactdriven, frequency upconverting coupled vibration energy harvesting device for low frequency operation,” Smart Materials and Structures, vol. 20, no. 4, Article ID 045004, 2011. View at: Publisher Site  Google Scholar
 A. F. Arrieta, P. Hagedorn, A. Erturk, and D. J. Inman, “A piezoelectric bistable plate for nonlinear broadband energy harvesting,” Applied Physics Letters, vol. 97, no. 10, Article ID 104102, 2010. View at: Publisher Site  Google Scholar
 S. C. Stanton, C. C. McGehee, and B. P. Mann, “Nonlinear dynamics for broadband energy harvesting: investigation of a bistable piezoelectric inertial generator,” Physica D: Nonlinear Phenomena, vol. 239, no. 10, pp. 640–653, 2010. View at: Publisher Site  Google Scholar
 M. Ferrari, V. Ferrari, M. Guizzetti, B. Andò, S. Baglio, and C. Trigona, “Improved energy harvesting from wideband vibrations by nonlinear piezoelectric converters,” Sensors and Actuators, A: Physical, vol. 162, no. 2, pp. 425–431, 2010. View at: Publisher Site  Google Scholar
 R. Torah, P. GlynneJones, M. Tudor, T. O'Donnell, S. Roy, and S. Beeby, “Selfpowered autonomous wireless sensor node using vibration energy harvesting,” Measurement Science and Technology, vol. 19, no. 12, Article ID 125202, 2008. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2015 Shuwen Zhang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.