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Article

The Effects of MnO2 Addition on the Physical Properties of Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3-Pb(Mg1/2W1/2)O3-BiFeO3 Ceramics

Department of Electrical Engineering, Semyung University, Jechon 390-711, Chungbuk, Korea
*
Author to whom correspondence should be addressed.
Submission received: 27 January 2021 / Revised: 26 February 2021 / Accepted: 5 March 2021 / Published: 9 March 2021

Abstract

:
In this paper, for the application to multi-layer piezoelectric devices capable of being used in piezoelectric speakers, Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3-BiFeO3 ceramics substituted with Pb(Mg1/2W1/2)O3 were manufactured according to MnO2 addition, and their physical properties were studied. At non-doped MnO2 added specimen, the maximum values of piezoelectric properties were shown, respectively: the εr of 2182, d33 of 513 pC/N, and kp of 0.634. When taking into consideration the low dielectric constant and high d33 in case of increasing the numbers of multilayer in ceramics, the x = 0.2 composition ceramics was suitable for the device application such as speaker using low-temperature sintering multilayer piezoelectric actuators.

1. Introduction

Recently, the regulations on hazardous substances have been strengthened. In particular, the manufacture and disposal of environmental pollutants have been severely restricted across all the electrical and electronic products. In the field of electronic ceramics, PZT system ceramics sintered above 1200 °C can cause in general the environmental pollution caused by PbO, which exhibits the rapid volatilization characteristics at around 1000 °C, because the PZT ceramics are composed of PbO over 60–70% [1,2,3,4]. Accordingly, in order to solve these problems, it is required to develop the low temperature sintering ceramics with high physical properties which can restrain the deteriorations of dielectric and piezoelectric properties in case of sintering at low temperature. Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3 ternary ceramics widely used as a compositions for piezoelectric speakers due to its large piezoelectric d33 constant can enhance piezoelectric properties through increasing the kp and d33 by the substitution of PMW or PZN instead of PNN [5,6,7,8]. Here, it is possible to sinter the ceramics at the temperature below 920 °C through the addition of sintering aids of ZnO, CuO, Li2CO3, and CaCO3.
Piezoelectric speakers have high sound pressure levels at high-frequency ranges, while they have low sound pressure levels at low-frequency ranges because of a solid state device. To increase the sound pressure at low frequencies, the frequency constant must be lowered, the number of stacked actuators must be increased in order to improve the generation power. Moreover, the piezoelectric d33 constant must be increased to increase the displacement. The composition ceramics applied to the LG G-8 smartphone has a rather high dielectric constant [1]. Such a high dielectric constant (εr) has caused a problem that a high power consumption is accompanied by an increase in capacitance (C) when the piezoelectric speaker is manufactured. In particular, when the piezoelectric speaker is made as a multi-layer type, the capacitance C value further can increase in proportion to the number of stacks, and the use of a material with a high dielectric constant can cause restrictions on the number of stacks because capacitance C is proportional to dielectric constant (εr). Therefore, to lower the dielectric constant of the ceramics is required. And also, for price competitiveness, pure Ag or Ag rich-Pd electrodes must be utilized [9,10,11]. Since the sintering temperature of the composition applied to the LG G-8 is currently 950 °C, Ag/Pd = 90/10 is used as an internal electrode. Therefore, the simultaneous firing process with Ag/Pd internal electrode should be applied during the lamination process for manufacturing the multilayer device. However, in this process, in order to use inexpensive pure Ag/Pd = 95/05 as an electrode, the sintering temperature of the ceramic must be 920 °C or less.
In addition, when the applied voltage is increased when driving the multilayer actuator, the sound pressure can increase, so it is good to increase the applied voltage while increasing the number of layers.
However, when the coercive electric field Ec is small, a de-poling problem in the multilayer actuator may occur, and the piezoelectric performance can be decreased.
Therefore, in order to prevent these phenomena, there is urgently required to develop the composition ceramics with a coercive electric field of 11 kV/cm or more.
For manufacturing the ceramics sintered at low temperature for multilayer piezoelectric device application, Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3-BiFeO3 composition ceramics substituted with Pb(Mg1/2W1/2)O3 with the piezoelectric d33 constant was selected and MnO2 was added, and their physical properties were studied.

2. Experimental

The samples were fabricated using a conventional mixed oxide process. The composition ceramics used in this experiment were as follows; 0.99[0.03Pb(Mg1/2W1/2)O3-0.09Pb(Ni1/3Nb2/3)O3-0.88Pb(Zr0.5Ti0.5)O3] + 0.01 BiFeO3 + 0.2 wt%Li2CO3 + 0.25wt% CaCO3 + x wt% MnO2 (x = 0 ~ 0.5).
The raw materials like PbO, ZrO2, TiO2, NiO, MnO2, Nb2O5, MgO, and WO3 for the above composition were weighted by mole ratio and the powders were ball-milled for 24 h. After drying, they were calcined at 850 °C for 2 h. And then, sintering aids CaCO3 and Li2CO3 were added, ball-milled, and dried. A 5% polyvinyl alcohol was added to the ceramic powders. The powders were molded by the pressure of 1 ton/cm2 in a mold which has a diameter of 17 millimeters, burned out at 600 °C for 3 h, and then sintered at 920 °C for 2 h. The density was measured using Archimedes method. For measuring the physical properties, the samples were polished and then electrodeposited with Ag paste. The poling was performed at 120 °C in a silicon oil bath by applying DC Electric Fields of 30 kV/cm for 30 min. The microstructure and crystal structure of samples were measured using a scanning electron microscope (SEM: Model Hitachi, S-2400) and X-ray diffraction (XRD: Rigaku, D/MAX-2500H), respectively. For investigating the dielectric properties, capacitance C was measured at 1 kHz using an ANDO AG-4034 LCR meter. For the purpose of investigating the piezoelectric characteristics, by using an impedance analyzer (Agilent 4294A), fr and fa were measured according to IRE standard, and then kp and Qm were calculated.

3. Results and Discussion

Figure 1 presents X-ray diffraction patterns of samples sintered at 920 °C with MnO2 addition. Pure perovskite phases were presented at all samples and no secondary phases are observed in the measurement range of XRD except for x = 0 and 0.1. As shown in Fig.1b, the ceramic specimens possess a weak rombohedral-tetragonal (R-T) phase coexistence from (002) and (200) peak along with the rhombohedral (200) peak between 40° and 50° from x = 0 to x = 0.3. Above x = 0.4, rombohedral phase appeared. Figure 2 presents the microstructure of samples sintered at 920 °C according to the amount of MnO2 addition. As can be seen in Figure 2, the average grain sizes gradually increased up to 6.13 μm at 0.1 wt% MnO2 with increasing MnO2 addition and then reduced over 0.2 wt% MnO2 addition.
Figure 3 shows density with MnO2 addition. The highest density of samples was increased up to 7.845 g/cm3 and 0.4 wt% MnO2 addition. Thereafter, the density was decreased due to the over addition of MnO2. These phenomena can be explained by the fact that the Mn 3+ ion can facilitate the particle diffusion by playing the role of acceptor dopant. Subsequently, the densification of specimens was enhanced [1].
Figure 4 shows kp according to MnO2 addition. The kp of samples increased according to the increase of the amount of MnO2 addition. The kp of samples showed the highest value of 0.634 at non doped MnO2 addition and then decreased due to acceptor dopant Mn 3+ ion.
Figure 5 presents d33 according to MnO2 addition. The d33 of samples decreased according to the increase of the amount of MnO2 addition. The d33 of samples showed the highest value of 513 (pC/N) at non doped MnO2 addition. It is considered that the Mn3+ ion can play a role of acceptor dopant by the substitution of Zr 4+ and Ti 4+ ion sites.
Figure 6 presents Qm according to MnO2 addition. The behavior of Qm showed opposite trends with kp. That is, as the amount of MnO2 addition increased, the value of Qm increased because the substitution of Mn 3+ ion for Zr 4+, Ti 4+ ion sites can increase the oxygen vacancy of the ceramics.
Figure 7 presents εr according to MnO2 addition. The εr of specimens decreased according to the increase of the amount of MnO2 addition and was nearly consistent with the trends of piezoelectric constant d33.
Figure 8 presents the temperature dependence of dielectric constant (εr) according to MnO2 addition. The Curie of specimens slowly decreased with the increase of the amount of MnO2 addition.
Taking into consideration the physical properties of εr = 1250, d33 = 347 pC/N, and kp = 0.605 were suitable for the device application such as speaker using low-temperature sintering multilayer piezoelectric actuators [1].
Table 1 shows the physical properties of specimens manufactured according to the amount of MnO2 addition.

4. Conclusions

For the application to multi-layer piezoelectric devices capable of being used in piezoelectric speakers, Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3-BiFeO3 ceramics substituted with Pb(Mg1/2W1/2)O3 were manufactured according to MnO2 addition, and their physical properties were studied. The results obtained from the experiments are as follows:
The ceramic composition showed weak rombohedral-tetragonal (R-T) phase coexistence from x = 0 to x = 0.3.
At non-doped MnO2 added specimen, the maximum values of piezoelectric properties were shown, respectively: the εr of 2182, d33 of 513 pC/N, and kp of 0.634. In case of increasing the numbers of multilayer in ceramics.
At x = 0.2 compositions, the εr of 1250, d33 of 347 pC/N, and kp of 0.605 were suitable for the device application such as speaker using low-temperature sintering multilayer piezoelectric actuators.

Author Contributions

Investigation, J.L.; Supervision, J.Y. Both authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Acknowledgments

This study was supported by 2020 Semyung University.

Conflicts of Interest

The authors declare no conflict of interest.

References

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Figure 1. XRD pattern with the amount of MnO2 addition (a) Wide range (b) Narrow range.
Figure 1. XRD pattern with the amount of MnO2 addition (a) Wide range (b) Narrow range.
Crystals 11 00269 g001
Figure 2. The SEM micrographs of the PMW-PNN-PZT with MnO2 addition (a) x = 0 wt% (b) x = 0.1 wt% (c) x = 0.2 wt% (d) x = 0.3 wt% (e) x = 0.4 wt% (f) x = 0.5 wt%.
Figure 2. The SEM micrographs of the PMW-PNN-PZT with MnO2 addition (a) x = 0 wt% (b) x = 0.1 wt% (c) x = 0.2 wt% (d) x = 0.3 wt% (e) x = 0.4 wt% (f) x = 0.5 wt%.
Crystals 11 00269 g002
Figure 3. Density with MnO2 addition.
Figure 3. Density with MnO2 addition.
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Figure 4. Electromechanical coupling factor (kp) with MnO2 addition.
Figure 4. Electromechanical coupling factor (kp) with MnO2 addition.
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Figure 5. Piezoelectric constant (d 33) with MnO2 addition.
Figure 5. Piezoelectric constant (d 33) with MnO2 addition.
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Figure 6. Mechanical quality factor (Qm) with MnO2 addition.
Figure 6. Mechanical quality factor (Qm) with MnO2 addition.
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Figure 7. Dielectric constant (εr) with MnO2 addition.
Figure 7. Dielectric constant (εr) with MnO2 addition.
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Figure 8. Temperature dependence of dielectric constant (εr) with MnO2 addition.
Figure 8. Temperature dependence of dielectric constant (εr) with MnO2 addition.
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Table 1. Physical properties with MnO2 addition.
Table 1. Physical properties with MnO2 addition.
XDensity [g/cm3]kpDielectric Constantd33
[pC/N]
g33
[mV·m/N]
QmTc (°C)
07.7880.634218251326.5554285
0.17.8060.561149535827.04193285
0.27.8230.605125034731.25195290
0.37.8280.60192628835.12356280
0.47.8450.58392727633.60426275
0.57.8080.60498229533.90274275
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Yoo, J.; Lee, J. The Effects of MnO2 Addition on the Physical Properties of Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3-Pb(Mg1/2W1/2)O3-BiFeO3 Ceramics. Crystals 2021, 11, 269. https://0-doi-org.brum.beds.ac.uk/10.3390/cryst11030269

AMA Style

Yoo J, Lee J. The Effects of MnO2 Addition on the Physical Properties of Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3-Pb(Mg1/2W1/2)O3-BiFeO3 Ceramics. Crystals. 2021; 11(3):269. https://0-doi-org.brum.beds.ac.uk/10.3390/cryst11030269

Chicago/Turabian Style

Yoo, Juhyun, and Jonghyun Lee. 2021. "The Effects of MnO2 Addition on the Physical Properties of Pb(Ni1/3Nb2/3)O3-Pb(Zr,Ti)O3-Pb(Mg1/2W1/2)O3-BiFeO3 Ceramics" Crystals 11, no. 3: 269. https://0-doi-org.brum.beds.ac.uk/10.3390/cryst11030269

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