Study of Dielectric and Piezoelectric Properties in the Ternary System Pb0.98Ca0.02[{(Zr0.52Ti0.48)0.98(Cr3+0.5 , Ta5+0.5)0.02}1–zPz]O3 Doping Effects
Hamzioui Louanes, Kahoul Fares, Abdessalem Nora, Boutarfaia Ahmed
.
DOI: 10.4236/msa.2012.31007   PDF    HTML   XML   4,077 Downloads   7,101 Views   Citations

Abstract

The effects of P2O5 oxide on microstructure, dielectric and piezoelectric properties of Pb0.98Ca0.02[{(Zr0.52Ti0.48)0.98( Cr3+1/2,Ta5+1/2)0.02}1–zPz]O3 ternary ceramics were investigated. Specimens with various contents of P2O5 from 0 to 12 wt. % were prepared by a conventional oxide mixing technique. The effect of P2O5 doping with regard to the development of the crystalline phase, density, microstructure, dielectric, ferroelectric and piezoelectric characteristics has been investigated. It has been found that the sintering temperature of piezoelectric Pb0.98Ca0.02[{(Zr0.52Ti0.48)0.98(Cr3+1/2,Ta5+1/2)0.02}1–zPz]O3 can be reduced by phosphorus addition without compromising the dielectric properties. A sintered density of 94 % of the theoretical density was obtained for 4 wt. % P2O5 addition after sintering at 1050°C for 4 h. Ceramics sintered at 1050°C with 4 wt. % P2O5 achieve excellent properties, which are as follows: kp = 0.73, ρ = 0.09 × 10+4 (Ω. cm), εr = 18800, tanδ = 0.0094 and Tc = 390°C.

Share and Cite:

H. Louanes, K. Fares, A. Nora and B. Ahmed, "Study of Dielectric and Piezoelectric Properties in the Ternary System Pb0.98Ca0.02[{(Zr0.52Ti0.48)0.98(Cr3+0.5 , Ta5+0.5)0.02}1–zPz]O3 Doping Effects," Materials Sciences and Applications, Vol. 3 No. 1, 2012, pp. 41-49. doi: 10.4236/msa.2012.31007.

1. Introduction

Lead-based perovskite-type solid solutions consisting of the ferroelectric and relaxor materials have attracted a growing fundamental and practical interest because of their excellent dielectric, piezoelectric and electrostrictive properties which are useful in actuating and sensing applications [1,2]. However, the sintering of PZT at high temperatures gives rise to a lead loss, which drastically degrades the device performance. Generally, a lead loss at high temperatures can be prevented by atmospherecontrolled sintering of PZT. However, such composition requires sintering at a high temperature (>1250˚C) in a controlled atmosphere to contain lead volatilization so as to avoid a shift in composition. To get around the problem, different sintering aids have been tried by various workers [3-5]. However, for practical applications, such sintering aids need proper selection so that the electrical and piezoelectric properties of the ceramics do not degrade.

The dielectric constants increased with the addition of NiO, Fe2O3, Gd2O3, Nb2O5 or WO3 and decreased with Cr2O3 or MnO2 addition [6-12]. Duran et al. studied the effect of MnO addition on the sintering and piezoelectric properties of Sm-modified lead titanate ceramics. The maximum density observed was 96.8% of the theoretical densit for 1% MnO addition at a sintering temperature of 1150˚C [13]. The main role of dopants is generally improved physical and mechanical properties of these materials. This work aims at, to study the influence of P2O5 on the properties dielectric and piezoelectric of a ceramics material of general formula: Pb0.98Ca0.02[(Zr0.52Ti0.48)0.98 (,)0.02]O3 and of structure perovskite.

2. Experimental Procedure

The compositions used for the present study were Pb0.98 Ca0.02[{(Zr0.52Ti0.48)0.98(,)0.02}1zPz]O3 with z varying as 0, 2, 4, 6, 8, 10 and 12 wt% respectively. The samples were prepared by a conventional oxide mixing technique. The appropriate amounts of PbO (99.9%), TiO2 (99.9%), ZrO2 (99.0%), Ta2O5 (99.9%), CaO (99.9%), Cr2O3 (99.9%) and P2O5 (99.9%) powders were weighed and mixed by ball milling with partially stabilized zirconia balls as media in isopropyl alcohol for 6 h. After drying, the mixture was calcined in a covered alumina crucible at 800˚C for 4 h. The calcined powders were again ball milled for 24 h. The resulting powders were uniaxially compacted into pellets of 10 mm in diameter at a pressure of 5 MPa, followed by isostatically pressing at 150 MPa. To investigate their sintering behavior, the specimens were sintered in a sealed alumina crucible at temperatures ranging from 1000˚C to 1180˚C for 2 h. To limit PbO loss from the pellets, a PbO-rich atmosphere was maintained by placing an equimolar mix ture of PbO and ZrO2 inside the crucible. The weight loss of a well-sintered specimen was less than 0.5 wt%, thus a 0.5 wt% excess PbO was added to compensate for the lead loss during sintering. The bulk density was measured using the Archimedean method. The sintered compounds are carefully ground, then analyzed by the scanning electron microscopy (SEM) is a technical for estimating the size distribution, the average size of grains after sintering and qualitatively assess the presence of porosity. The micrographics are made using a Microscope JMS 6400. To investigate the electrical properties, the sintered disks were lapped on their major faces, and then sliver electrodes were deposited with a low temperature paste at 700˚C for 30 min. The piezoelectric samples were poled in a silicone oil bath at 100˚C by applying 20 kV/cm for 20 min. then cooling them under the same electric field. They were aged for 24 h prior to testing. The temperature dependence of dielectric properties was measured at temperatures ranging from room temperature to 420˚C with a heating rate of 2 ˚C/min using an impedance analyzer—HP4192A, Hewlett-Packard, Palo Alto, CA. The electromechanical coupling factor, kp, was determined by the resonance and antiresonance technique using another impendence analyzer (SI1260 Impedance/Gain-Phase Analyzer, Solartron, UK). (kp = [2.51(fa – fr)/fr)]1/2, where fr and fa are the resonance and anti-resonance frequencies, respectively [14]. Variation of the dielectric constant εr, resistivity and also the angle of the losses were examined by using a measuring bridge type RLC (bridge Schering) depending on temperature, concentration, the frequency.

3. Results and Discussion

3.1. Sintered Density

Figure 1(a) shows the variation of density with sintering temperature and the amount of P2O5 addition. This curves show the similar variation trend with increasing sintering temperature. The density of specimens sintered at 1050˚C showed the maximum value of 7.52 g·cm3 at 4 wt% P2O5 and then was decreased after the maximum value. This variation is mainly attributed to the formation of liquid phase of excess PbO that improves densification of

Conflicts of Interest

The authors declare no conflicts of interest.

References

[1] G. H. Haertling, “Ferroelectric Ceramics: History and Technology,” Journal American Ceramic Society, Vol. 82, No. 4, 1999, pp. 797-818. doi:10.1111/j.1151-2916.1999.tb01840.x
[2] K. Uchino, “Ferroelectric Device,” Marcel Dekker, New York, 2000.
[3] S. Y. Cheng, S. L. Fu, C. C. Wei and G. M. Ke, “The Properties Low-Temperature Fixed Piezoelectric Ceramics,” Journal of Materials Science, Vol. 21, No. 2, 1986, pp. 571-576. doi:10.1007/BF01145525
[4] H. G. Lee, J. H. Choi and E. S. Kim, ” Low-Temperature Sintering and Electrical Properties of (1?x)Pb(Zr0.5Ti0.5) O3-xPb(Cu0.33Nb0.67)O3 Ceramics,” Journal of Electroceramics, Vol. 17, No. 2-4, 2006, pp. 1035-1040. doi:10.1007/s10832-006-0384-1
[5] R. Mazumder, A. Sen and H. S. Maiti, “Impedance and Piezoelectric Constants of Phosphorous-Incorporated Pb (Zr0.52Ti0.48)O3 Ceramics,” Materials Letters, Vol. 58, No. 25, 2004, pp. 3201-3205. doi:10.1016/j.matlet.2004.06.011
[6] G. Robert, M. D. Maeder, D. Damjanovic and N. Setter, “Synthesis of Lead Nickel-Niobate Zirconate Titanate Solid Solutions by a B-Site Precursor,” Journal American Ceramic Society,” Vol. 84, No. 12, 2001, pp. 2863-2868. doi:10.1111/j.1151-2916.2001.tb01107.x
[7] L. Pdungsap, S. Boonyeun, P. Winotai, N. Udomkan and P. Limsuwan, “Effects of Gd3+ Doping on Structural and Dielectric Properties of PZT (Zr:Ti = 52:48) Piezoceramics,” The European Physical Journal B, Vol. 48, No. 3, 2005, pp. 367-372. doi:10.1140/epjb/e2005-00407-9
[8] S. J. Yoon, A. Joshi and K. Uchino, “Effect of Additives on the Electromechanical Properties of Pb(Zr,Ti)O3-Pb-(Y2/3W1/3<、su>)O3 Ceramics,” Journal of the American Cera- mic Society, Vol. 80, No. 4, 2005, pp. 1035-1039. doi:10.1111/j.1151-2916.1997.tb02942.x
[9] G. A. Smolenskii and A. I. Agranovskaya, “Dielectric Po- larization of a Number of Complex Compounds,” Soviet Physics Solid State, Vol. 1, No. 10, 1960, pp. 1429-1437.
[10] F. Kulcsar, “Electromechanical Properties of Lead Titanate Zirconate Ceramics Modified with Tungsten and Thorium,” Journal American Ceramic Society, Vol. 48, No. 1, 1965, pp. 48-54. doi:10.1111/j.1151-2916.1965.tb11796.x
[11] N. Abdessalem and A. Boutarfaia, “Effect of Composition on the Electromechanical Properties of Pb[ZrxTi(0.9-x)- (Cr1/5, Zn1/5, Sb3/5)0.1]O3 Ceramics,” Ceramics International, Vol. 33, No. 2, 2007, pp. 293-296. doi:10.1016/j.ceramint.2005.08.008
[12] J. S. Kim and K. H. Yoon, “Physical and Electrical Properties of MnO2-Doped Pb(ZrxTi1?x)O3 Ceramics,” Journal of Materials Science, Vol. 29, No. 3, 1994, pp. 809-815. doi:10.1007/BF00445997
[13] P. Duran, J. F. Fernandez and C. Moure, “Effect of MnO Additions on the Sintering and Piezoelectric Properties of Samarium-Modified Lead Titanate Ceramics,” Journal of Materials Science Letters, Vol. 10, No. 15, 1991, pp. 917-919. doi:10.1007/BF00724781
[14] Z. He, J. Ma, R. Z. Hang, “Investigation on the Microstructure and Ferroelectric Properties of Porous PZT Ceramics,” Ceramics International, Vol. 30, No. 7, 2004, pp. 1353-1356. doi:10.1016/j.ceramint.2003.12.108
[15] R. Sumang and T. Bongkarn, “The Effect of Excess PbO on Crystal Structure, Microstructure, Phase Transition and Dielectric Properties of (Pb0.75 Sr0.25)TiO3 Ceramics,” Taylor & Francis Group LLC, Vol. 403, No. 1, 2010 , pp. 82-90. doi:10.1080/00150191003748949
[16] P. Goel, S. Sharma, K. L. Yadav and A. R. James, “Structural and Dielectric Properties of Phosphorous-Doped PLZT Ceramics,” Pramanas, Vol. 65, No. 6, 2005, pp. 1127-1132. doi:10.1007/BF02705288
[17] A. K. Saha, D. Kumar, O. Parkash, A. Sen and H. S. Maiti, “Effect of Phosphorus Addition on the Sintering and Dielectric Properties of Pb(Zr0.52Ti0.48)O3,” Materials Research Bulletin, Vol. 38, No. 7, 2003, pp. 1165-1174. doi:10.1016/S0025-5408(03)00112-0
[18] O. Ohtaka, R. Von Der Mühll and J. Ravez, “Low-Temperature Sintering of Pb(Zr,Ti)O3 Ceramics with the Aid of Oxyfluoride Additive: X-Ray Diffraction and Dielectric Studies,” Journal American Ceramic Society, Vol. 78, No. 3, 1995, pp. 805-808. doi:10.1111/j.1151-2916.1995.tb08251.x
[19] W. Heywang, “Ferroelektrizit?t in Perowskitischen Systemen und Ihre Technischen Anwendungen,” Zeitschrif Angewandte Physik, Vol. 19, 1965, pp. 473-481.
[20] S. Babu, D. Singh and A. Govindan, “Electrical Properties of Calcium Modified PZT System,” International Journal of Computer Science et Technologie, Vol. 2, No. 1, 2011, pp. 128-131.
[21] IEEE Standard on Piezoelectricity, IEEE Standard 176-1978, Institute of Electrical and Electronic Engineers, New York, 1978.

Copyright © 2024 by authors and Scientific Research Publishing Inc.

Creative Commons License

This work and the related PDF file are licensed under a Creative Commons Attribution 4.0 International License.