Physics Research International

Physics Research International / 2011 / Article

Research Article | Open Access

Volume 2011 |Article ID 395182 |

Peng Qi, Juan Du, Guozhong Zang, "Sintering and Characterization of (Li, Sb, Ta)-Modified (Na, K)NbO3 Lead-Free Ceramics", Physics Research International, vol. 2011, Article ID 395182, 5 pages, 2011.

Sintering and Characterization of (Li, Sb, Ta)-Modified (Na, K)NbO3 Lead-Free Ceramics

Academic Editor: Sergey B Mirov
Received28 Apr 2011
Accepted07 Jul 2011
Published08 Sep 2011


Lead-free alkaline niobate-based piezoceramics, (Na0.52K0.435Li0.045)Nb0.87Sb0.08Ta0.05O3 (abbreviated KNLNT-S8), were prepared by conventional solid-state sintering method. The effects of sintering temperature on microstructure and piezoelectric properties of the (Li, Sb, Ta)-modified (Na, K) NbO3 were investigated. Microstructure of the samples sintered at different temperatures was observed by scanning electron microscopy (SEM) and optical microscopy. The KNLNT-S8 sample sintered at 1100°C possessed highest piezoelectric constant and high-field piezoelectric strain coefficient of 332 pC/N and 530 pm/V, respectively, with electromechanical coupling factors of 0.52 and of 0.48.

1. Introduction

Lead zirconium-titanate solid solution, PZT, has been in the leading position in piezoceramics for half a century because of its excellent piezoelectric properties. although, the content of PbO in PZT is higher than 60 wt%, the Pb volatilization during sintering process and the discarded PZT products pollute the environment and do harm to human health. Therefore, it is an urgent task developing environment-friendly industrial piezoceramics products. Among several families of lead-free piezoelectric materials, (K, Na)NbO3 (KNN) system has been considered a good candidate for PZT alternative material owing to its strong piezoelectricity. However, it is difficult to prepare well-densified KNN ceramics because of the volatilization of potassium and its reactivity with moisture [13]. KNN modified by other compound has been studied in order to improve this piezoelectric properties and sintering performance [47].

In our previous research, the morphotropic phase boundary (MPB) of (Na0.52K0.48-xLix)Nb1-x-ySbxTayO3 was identified and (Na0.52K0.435Li0.045)Nb0.905Sb0.045Ta0.05O3 was found to have a high piezoelectric constant of 308 pC/N [8]. In this paper, more Sb was introduced near the MPB composition, to form (Na0.52K0.435Li0.045)Nb0.87Sb0.08Ta0.05O3 (KNLNT-S8) piezoceramics with a further improved piezoelectric constant (332 pC/N). The sintering effects on properties of the (Li, Sb, Ta)-modified (Na, K)NbO3 were investigated.

2. Experimental

Chemical composition of our samples in this study was (Na0.52K0.435Li0.045)Nb0.87Sb0.08 Ta0.05O3. Analytical-grade Na2CO3 (99.8%), K2CO3 (99.5%), Li2CO3 (99.9%), Nb2O5 (99.8%), Ta2O5 (99.8%), and Sb2O5 (99.9%) were used as starting materials. With a ratio to alcohol of 1 : 1.3, the chemicals were wet-milled in polyethylene bottles with ZrO2 balls as milling media for 12 h. The milled slurry was dried and pressed into discs of 30 mm in diameter. The discs were calcined at 880–920°C for 3–5 h. The calcined discs were crushed and ball-milled again for 12 h. The dried powder was mixed with 0.5% weight PVA binder and pressed into discs of 15 mm in diameter and 1.2 mm in thickness at 160 MPa. After burning out the PVA at 650°C, the discs were put into Al2O3 crucibles and sintered at 1070–1120°C for 3–6 h. Silver paste was applied on faces of the sintered discs to form electrodes by firing at 550°C, and then the samples were poled in silicon oil at 30°C for 15 min under a DC field of 4.0 kV/mm. Piezoelectric constants were determined by using Berlincourt-type quasistatic meter at 50 Hz. High-field piezoelectric strain coefficient, , was calculated from the slope of the field-induced strain curves. Electromechanical coupling coefficients, and , were determined by a resonance and antiresonance method according to IEEE standards by using an impedance analyzer (Agilent 4294A). Sample surface microstructure was observed by using a scanning electron microscopy (SEM), and the polished surface morphology was observed by using an optical microscopy. Polarization hysteresis and strain-electric field curves were measured by using a modified Sawyer-Tower circuit and linear variable differential transducer (LVDT) driven by a lock-in amplifier (Stanford Research Systems, Model SR 830).

3. Results and Discussion

In order to obtain high-density KNN-based ceramics, it is necessary to consider the volatility of sodium and potassium [9]. Figure 1(a) shows density and dielectric loss of the KNLNT-S8 ceramics as a function of sintering temperature. The density of the KNLNT-S8 ceramics increases with increasing sintering temperature from 1070 to 1100°C and reaches its maximum of 4.49 g/cm (relative density over 96%) at 1110°C. As all samples were sintered in covered Al2O3 crucibles and embedded in powder with the same composition, the volatility of sodium and potassium was suppressed effectively at sintering temperatures of 1110°C. As the sintering temperature exceeds 1120°C, density of the KNLNT-S8 sample decreases owing to the excessive volatility of sodium and potassium. Dielectric loss of the KNLNT-S8 ceramics keeps to be about 2.0% when the sintering temperature varies from 1080 to 1110°C, much lower than that (~13%) of the sample sintered at 1070°C. Piezoelectric properties of the KNLNT-S8 ceramics as a function of sintering temperature are shown in Figure 1(b). The piezoelectric constant, , and electromechanical coupling factors, and , reach their maximum values of 332 pC/N, 0.52 and 0.48, respectively, at 1100°C. However, the high-field piezoelectric strain coefficient keeps its maximum value in a very wide temperature range from 1080 to 1100°C. This property makes KNLNT-S8 system a good candidate in terms of industrial production.

Figure 2 shows surface SEM images of the KNLNT-S8 ceramics sintered at 1080°C, 1100°C, and 1120°C. The sample sintered at 1080°C has grains with a wide size distribution. As the sintering temperature is raised to 1100°C, it can be seen that brick-like shaped grains congregate closely and become homogeneous. Uniform grain microstructure is beneficial to enhancing the mechanical strength of piezoelectric ceramics [10]. However, as the sintering temperature exceeds 1120°C, pores and abnormal grains appear in the ceramics, which may be attributed to the volatilization and segregation of the alkaline elements.

Optical microscopy images of the polished samples are shown in Figure 3. Many abnormally huge pores are observed in the samples sintered at 1080°C and 1120°C, indicating that the sample was not fully identified at low temperature while much alkaline elements volatilized at high temperature. For the sample sintered at 1100°C, the pores are smaller in size and distributed regularly, showing good compactness. This result is in a good agreement with the density curve (Figure 1(a)).

Figure 4 shows hysteresis loops of the KNLNT-S8 ceramics sintered at 1080, 1100, and 1110°C. The samples sintered between 1080°C and 1110°C have good ferroelectric properties with a high remanent polarization of 22 μC/cm2 and a coercive field of 21 kV/cm. For samples sintered below 1070°C or over 1120°C, it is difficult to obtain closed hysteresis loops because of their high conductivity and defects. It is worth noting that coercive field of the KNLNT-S8 ceramics (~21 kV/cm) is higher than the value of pure KNN (~8 kV/cm) [14], demonstrating a hardening effect. Unipolar field-induced strain of the KNLNT-S8 ceramics sintered at 1100°C is shown in Figure 5. The sample exhibits very high electric-field-induced strain; the value of high-field piezoelectric strain coefficient is as high as 530 pm/V for the 10–20 kV/cm induced strain curve. The high makes this system a promising lead-free piezoceramics for high-power actuator devices applications.

Table 1 shows piezoelectric and dielectric properties of the KNLNT-S8 ceramics sintered at 1100°C and some KNN-based ceramics reported previously. It is found that our KNLNT-S8 ceramics have excellent piezoelectric and electromechanical properties, such as high piezoelectric constant of 332 pC/N, low dielectric loss of about 2.0%, high electromechanical planar coupling coefficient of 0.52, and thickness coupling coefficient of 0.48. Compared to (Na0.52K0.435Li0.045)Nb0.905Sb0.045Ta0.05O3 ceramics [8], high Sb content led to improved piezoelectric properties.

Compositions (pC/N) (pm/V) tan δ (%)

332 530 2.0 1210 0.52 0.48
[8] 308 490 1.9 1009 0.51 0.47
[11] 300 400
[12]328 702 0.48
[13]3213.6 1780 0.52

4. Conclusions

In conclusion, high-performance lead-free (Na0.52K0.435Li0.045)Nb0.87Sb0.08Ta0.05O3 piezoceramics have been synthesized by the conventional mixed oxide route. The sintering effects on piezoelectric properties and microstructure of (Li, Sb, Ta)-modified (Na, K)NbO3 ceramics have been studied systematically. The KNLNT-S8 ceramics sintered at 1100°C had the lowest porosity and the highest density of 4.49 g/cm, piezoelectric constant of 332 pC/N, and a dielectric loss of about 2.0%. In particular, the sample possessed good high-field piezoelectric strain effects, with a value of 530 pm/V, making it promising candidate for practical application.


The authors deeply acknowledge the financial support of the National Natural Science Foundation of China (no. 50802038).


  1. Y. Liu, Y. Huang, T. Liu, B. Zhang, Q. Yan, and G. Zhang, “Dielectric and piezoelectric properties of (1 - x)(K0.498Na0.498Li0.04)NbO3x(Bi0.5Na0.5)0.9Ba0.1(Zr0.0055 Ti0.9945)O3 lead-free ceramics,” Journal of Materials Science, vol. 45, no. 1, pp. 188–191, 2010. View at: Publisher Site | Google Scholar
  2. J. Li, Q. Sun, and W. Ma, “Molten salt synthesis of (K0.47Na0.47Li0.06) NbO3 lead-free piezoelectric ceramics,” Transactions of Tianjin University, vol. 16, no. 2, pp. 152–155, 2010. View at: Publisher Site | Google Scholar
  3. S. J. Liu, B. Wan, P. Wang, and S. H. Song, “Influence of A-site non-stoichiometry on structure and electrical properties of K0.5Na0.5NbO3-based lead-free piezoelectric ceramics,” Scripta Materialia, vol. 63, no. 1, pp. 124–127, 2010. View at: Publisher Site | Google Scholar
  4. Y. Zhou, M. Guo, C. Zhang, and M. Zhang, “Hydrothermal synthesis and piezoelectric property of Ta-doping K0.5Na0.5NbO3 lead-free piezoelectric ceramic,” Ceramics International, vol. 35, no. 8, pp. 3253–3258, 2009. View at: Publisher Site | Google Scholar
  5. D. Lin, Q. Zheng, K. W. Kwok, C. Xu, and C. Yang, “Dielectric and piezoelectric properties of MnO2-doped K0.5Na0.5Nb0.92Sb0.08O3 lead-free ceramics,” Journal of Materials Science: Materials in Electronics, vol. 21, no. 7, pp. 649–655, 2010. View at: Publisher Site | Google Scholar
  6. F. Azough, M. Wegrzyn, R. Freer, S. Sharma, and D. Hall, “Microstructure and piezoelectric properties of CuO added (K, Na, Li)NbO3 lead-free piezoelectric ceramics,” Journal of the European Ceramic Society, vol. 31, no. 4, pp. 569–576, 2011. View at: Publisher Site | Google Scholar
  7. K. C. Singh and C. Jiten, “Lead-free piezoelectric ceramics manufactured from tantalum-substituted potassium sodium niobate nanopowders,” Materials Letters, vol. 65, no. 1, pp. 85–88, 2011. View at: Publisher Site | Google Scholar
  8. B. Q. Ming, J. F. Wang, P. Qi, and G. Z. Zang, “Piezoelectric properties of (Li, Sb, Ta) modified (Na,K) NbO3 lead-free ceramics,” Journal of Applied Physics, vol. 101, no. 5, Article ID 054103, 2007. View at: Publisher Site | Google Scholar
  9. P. Zhao, B. P. Zhang, and J. F. Li, “High piezoelectric d33 coefficient in Li-modified lead-free (Na,K) NbO3 ceramics sintered at optimal temperature,” Applied Physics Letters, vol. 90, no. 24, Article ID 242909, 2007. View at: Publisher Site | Google Scholar
  10. C. A. Randall, N. Kim, J. P. Kucera, W. Cao, and T. R. Shrout, “Intrinsic and extrinsic size effects in fine-grained morphotropic-phase-boundary lead zirconate titanate ceramics,” Journal of the American Ceramic Society, vol. 81, no. 3, pp. 677–688, 1998. View at: Google Scholar
  11. Y. Saito, H. Takao, T. Tani et al., “Lead-free piezoceramics,” Nature, vol. 432, no. 7013, pp. 84–87, 2004. View at: Publisher Site | Google Scholar
  12. R. Zuo and C. Ye, “Structures and piezoelectric properties of (NaKLi)1−x (BiNaBa)x Nb1−x Tix O3 lead-free ceramics,” Applied Physics Letters, vol. 91, no. 6, Article ID 062916, 2007. View at: Publisher Site | Google Scholar
  13. J. Fu, R. Zuo, D. Lv, Y. Liu, and Y. Wu, “Structure and piezoelectric properties of lead-free (Na0.52K0.44x)(Nb0.95xSb0.05O3xLiTaO3 ceramics,” Journal of Materials Science: Materials in Electronics, vol. 21, no. 3, pp. 241–245, 2010. View at: Publisher Site | Google Scholar
  14. G. H. Haertling, “Properties of hot-pressed ferroelectric alkali niobate ceramics,” Journal of the American Ceramic Society, vol. 50, no. 6, pp. 329–330, 1967. View at: Google Scholar

Copyright © 2011 Peng Qi 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.

Related articles

No related content is available yet for this article.
 PDF Download Citation Citation
 Download other formatsMore
 Order printed copiesOrder

Related articles

No related content is available yet for this article.

Article of the Year Award: Outstanding research contributions of 2021, as selected by our Chief Editors. Read the winning articles.