Acceleration and frequency of the vibration sources in the environment [13].
Abstract
The piezoelectric material selection and the circuit design in vibrational energy harvesting are discussed. The performances of the energy-harvesting unimorph devices that captured frequencies of 60 Hz by using piezoelectric PZT-based and BT-based ceramics were evaluated. Output voltages and power from the devices depend on the amplitude and the frequency of the oscillations, and depend on the load resistance. Generally, PZT-based ceramics are superior for piezoelectric energy-harvesting applications. The figures of merit of the materials are discussed in order to provide the guidelines of the piezoelectric material selections. Piezoelectric voltage coefficient, g31, is considered to be good parameter to predict the maximum voltages. On the other hand, d31g31/tanδ, k312Qm and d31g31 are close to the behavior of the maximum power. Combination of the piezoelectric unimorph and power management circuit produced the constant voltage output, which would be used as the power sources.
Keywords
- energy harvesting
- piezoelectricity
- lead-free
- power management circuit
1. Introduction
Energy harvesting (EH) is the process of capturing small amounts of energy from external natural energy sources, accumulating and storing them for later use. In many cases, EH devices convert ambient energy into electrical energy. By combining suitable electronics, EH devices can be used for creating a self-sufficient energy supply system. The merits of the system include the replacement or supplement of the batteries and the minimization of the associated maintenance expenditure, and the replacement of the power supply cables. Major application target of EH is for independent sensor networks [1]. The aspect of the sensor network is illustrated in Figure 1. The sensor network is consisted of the wireless sensors placed on various places, such as human body, vehicles, and buildings, in order to monitor the physical or environmental conditions, such as temperature, humidity, sound, pressure, etc. The data are gathered from the sensor nodes to data center through the gateway sensor node. The compositions of the sensor node are illustrated in the upper right side of Figure 1. Sensor node is consisted with a radio transceiver with an antenna, a microcontroller, an electronic circuit for interfacing with the sensors, and an energy source. EH is attracting an attention for the embedded energy source of sensor nodes and is considered to be one of the key technologies of Internet of things (IoT). In the last decade, the field of EH has increasingly become important as illustrated in the rising numbers of publications in Figure 2.
The available energy from the environment includes solar power, thermal energy, wind energy, salinity gradients, and kinetic energy. Solar energy has the capability of providing large power density outdoors; however, it is not easy to capture the adequate solar energy in indoor environment. Mechanical vibration is the most attractive alternative [1, 2]. Vibration-electrical energy harvesting using piezoelectric effects has been explored for possible use in sensor network modules [1–11]. In order to harvest energy from the environment, it is necessary to capture vibrations with frequencies less than 200 Hz, because such frequencies are dominant in normal life and in vehicles, as shown in Table 1 [12, 13].
Origin of the vibrations | Acceleration (m2/s) | Frequency (Hz) |
---|---|---|
3-Axis machine | 10 | 70 |
Cooking mixer | 6.4 | 121 |
Clothes dryer | 3.5 | 121 |
Electric oven (small size) | 2.25 | 121 |
Air exhaust in buildings | 0.2-1.5 | 60 |
Wood deck with traffic | 1.3 | 385 |
Windows facing busy street | 0.7 | 100 |
Note PC loading CD | 0.6 | 75 |
Washing machine | 0.5 | 109 |
Refrigerator | 0.1 | 241 |
Considering the application to the power source, appropriate power management circuit design to adjust to the requirement of the application devices. The block diagram of the vibrational energy-harvesting systems is illustrated in Figure 3. Energy harvester is vibrated by the excitation force of the vibration source, then the mechanical energy is converted to electrical energy by piezoelectrics in energy harvester. The generated electrical energy is consumed in the application circuits; finally, the optimum control of an electrical output in accordance with a load condition of the applications is required. Therefore, the power management circuit plays an important role in the system. The block diagram of the power management circuit is shown in Figure 4. Since the voltage and current of the electricity generated by the piezoelectric energy harvester are alternating, diode rectifier has required to produce direct current (DC) power supply. And the electricity from the piezoelectric power generator is large amplitude and frequency fluctuations; therefore, regulation circuit is required. DC-DC convertor is controlled by regulation circuit to adjust the requirement of the applications. The output voltage from the piezoelectric generator, the output voltage after rectification, and the controlled voltage output are shown in Figure 5(a–c), respectively. Alternating voltage having a waveform of almost positive negative symmetry is generated by piezoelectric generator. By full wave rectifying circuit, the generated voltage was converted to one of constant polarity (positive or negative). Smoothing capacitor or filter is required to produce the steady direct voltage. The regulated circuit including capacitor and DC-DC convertor produced constant voltage output. In order to enhance the performance of the energy-harvesting circuit, a nonlinear processing technique “synchronized switch harvesting on inductor” (SSHI) [5], or active full-wave rectifier by using CMOS (complementary metal oxide semiconductor) technology [14], and power conditioning circuit with maximum power point tracking (MMPT) have been proposed [15].
In order to obtain energy harvesters with high performances, material selections are important problems. From the view point, figures of merit of the materials have been discussed thus far. Priya has provided dimensionless figures of merit (DFOM) for a 3–1 mode transducer under on-resonance and off-resonance conditions, as follows.
DFOM = (
DFOM = (
Here,
Takeda et al. have suggested that power output from vibration-based generators should be expressed as linear functions of the term composed of electromechanical coupling coefficients
In our previous study [16, 17] the unimorphs—cantilevers with an active piezoelectric layer and an inactive elastic layer—were fabricated, and, prelaminar results on the performance were reported. Although EH devices fabricated by using thin film piezoelectrics are advantageous in the miniaturization and mass-productivity, EH devices fabricated by using bulk ceramics are superior in power output. Moreover, in the case of the unimorph EH devices by using bulk ceramics, material selections are easy by just replacing the ceramics. While, in the case of EH devices by using thin films, film deposition process is depending on the materials, comparative study of materials is relatively difficult. From the perspective of minimizing the environmental load by avoiding the use of lead-containing materials, consideration of lead-free piezoelectric materials is valuable for energy-harvesting devices [13]. Therefore, in addition to PZT-based ceramics, barium titanate (BT)-based ceramics was evaluated for piezoelectric materials in this chapter. The performance of piezoelectric energy-harvesting devices that captured frequencies of 60 Hz for PZT-based and BT-based ceramics was evaluated and the figures of merit of the materials have been discussed in order to provide the guidelines of the piezoelectric material selections. The results using power management circuit are included for evaluating the performance as the power source.
2. Experimental
The commercial piezoelectric bimorph is used for basic operations in the power management circuit. And the piezoelectric unimorph were fabricated by remodeling the commercial bimorphs. The experimental setup for measuring the unimorph generator is shown in Figure 6. Details were described in our previous study [16]. Commercial bimorph was produced by using a patterned fiber-reinforced plastic (FRP) plate (105 mm × 10 mm × 1.6 mm) that was used as the base beam. Piezoelectric ceramics was adhered to both the side of the beam. The unimorph structure was fabricated by removing the piezoelectric ceramics from both the side and adhering PZT- or BT-based ceramics (10 mm × 18 × 0.5 mm) to one side of the FRP beam. The unimorph was attached to the vibration generator and oscillated with various frequencies and accelerations. And the characteristic frequency of the beam was 57 Hz. An acceleration sensor was attached to the other end, and the displacements of the unimorph were monitored during measurement. The beam vibrated with the tip as a node at 60 Hz.
In the case of the unimorphs, commercial bulk PZT ceramic disks were used. The PZT-based ceramic disks were hard PZT ceramics with Tc of 325°C, soft PZT ceramics with Tc of 145, 190, or 330°C (hereafter PZTh325, PZTs145, PZTs190, or PZTs330, hereafter, respectively, NEC Tokin) of 0.5 mm thickness were used [15]. As lead-free ceramics, nondoped BaTiO3 (BT) ceramics, manganum-doped BaTiO3 (BT-Mn), and (Ba0.85Ca0.15)(Ti0.95Zr0.05)O3 (BCCZ5) sintered at 1400°C, 1300°C, and 1350°C, respectively, were used. The dielectric and piezoelectric properties of these ceramics are shown in Table 2 and were reported in detail in our previous study [16, 18].
Samples | Dielectric constant | Maximum voltage (V) | Maximum power (μW) | ||||
---|---|---|---|---|---|---|---|
PZTh325 | 1190 | 461 | 35.3 | 11.8 | 347 | 19.6 | 19.2 |
PZTs145 | 4940 | 66.7 | 34.4 | 6.2 | 507 | 18.4 | 72.2 |
PZTs190 | 3578 | 64.8 | 32.8 | 7.1 | 445 | 38 | 351 |
PZTs330 | 1509 | 71.4 | 36.3 | 11.9 | 370 | 56 | 307 |
BT | 3173 | 51.9 | 18.8 | 4.1 | 158 | 2.6 | 0.8 |
BT-Mn | 3635 | 95.3 | 11.7 | 2.2 | 85 | 11 | 24.5 |
BCCZ5 | 1867 | 66.3 | 12.4 | 2.6 | 63 | 9.8 | 17 |
In order to evaluate the performance as an energy source, a piezoelectric energy-harvesting power supply integrated circuit (LTC3588-1, Linear Technology Corp.) that integrates a low-loss full-wave bridge rectifier with a high efficiency buck converter was employed [19]. The bimorphs were oscillated for 45 sec. In this power supply circuit,
3. Results and discussion
The frequency dependence of the Vcharge from the piezoelectric unimorph is shown in Figure 7. The Vcharge shows the maximum at 57 Hz, indicating that the maximum displacement of the bimorph provides the largest voltage output. The output voltages across the various load resistors were measured. Figure 8 shows the load voltage delivered to load resistance by oscillating the unimorph with a relative displacement of 0.2, 0.4, and 0.8 mm and a frequency of 60 Hz. It is found that the voltage increases proportionally to the relative displacement. From the voltage, the output electric powers, P, at the load resistance were calculated using P=1/2(V2/R) equation. The results are shown in Figure 9. It is noted that the electric powers varied with the load resistance. In all samples, the power increases with increasing resistance and showed that their peak power decreases with increasing resistance. The resistance that yielded maximum power varied with the samples, this resistance roughly correspond to the resistance of the samples. These results were very close to our previous results; however, the hard PZT ceramics yielded higher output voltage but smaller power in this study. The reason for this phenomenon is not yet clear. In the case of the hard PZT, the electrical damping may be larger [13]. Unimorph that used PZT with higher Tc generates larger voltage and power. Concerning generators that used BT ceramics, Mn-doping was effective. Mn-addition raises
The charging voltage (
Samples | Maximum voltage (V) | Maximum power (μW) | Energy (μJ) | Pgood (s) |
---|---|---|---|---|
PZTh325 | 19.6 | 19.2 | 233 | 0 |
PZTs145 | 18.4 | 72.2 | 423 | 38 |
PZTs190 | 38 | 351 | 2753 | 56 |
PZTs330 | 56 | 307 | 3493 | 55 |
BT | 2.6 | 0.8 | 16 | 0 |
BT-Mn | 11 | 24.5 | 194 | 0 |
BCCZ5 | 9.8 | 17 | 135 | 0 |
4. Conclusion
The performance of piezoelectric energy-harvesting devices fabricated from the base FRP beam and PZT-based and BT-based ceramics that captured frequencies of 60 Hz was evaluated. The output voltage from the generator is proportional to the displacement of the piezoelectric ceramics. And the output voltages from the bimorph and unimorph generator varied with the applied frequencies. The output voltage increased with the load resistance, on the other hand, the output power showed the maximum at around the load resistance with the impedance of the piezoelectric generators. And the figures of merit of the materials have been discussed in order to provide the guidelines of the piezoelectric material selections. Piezoelectric voltage coefficient,
Acknowledgments
This study was supported in part by a grant from JSAP KAKENHI Grant Number 26420684, and a Green Network of Excellence (GRENE) project grant from the Ministry of Education, Culture, Sports, Science, and Technology, Japan. And part of figures and tables are reprinted with permission from Taylor and Francis.
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