Elsevier

Ceramics International

Volume 40, Issue 7, Part B, August 2014, Pages 11269-11276
Ceramics International

Electrocaloric effects in spark plasma sintered Ba0.7Sr0.3TiO3-based ceramics: Effects of domain sizes and phase constitution

https://doi.org/10.1016/j.ceramint.2014.03.175Get rights and content

Abstract

The crystal structures, domain structures, dielectric strengths and electrocaloric effects of spark plasma sintered Ba0.7Sr0.3TiO3 and Ba0.7Sr0.3Ti0.997Mn0.003O3 ceramics have been investigated. The densification can be enhanced by the spark plasma sintering (SPS) process without obvious grain growth, where the fine ferroelectric domain structures are obtained. The content of tetragonal phase in Ba0.7Sr0.3TiO3 ceramics prepared by the SPS process is lower than that in the counterpart prepared by the conventionally sintering process, but it will increase again by partially substituting titanium with 0.3 mol% manganese ions. The dielectric strength can be significantly enhanced by the spark plasma sintering process, which can be improved further by Mn-substitution, and consequently the electrocaloric temperature change, ΔT, increases. Meanwhile, the electrocaloric strength has been enhanced by the spark plasma sintering process, which should be attributed to combined effects of domain wall density the content of ferroelectric phase in the present ceramics.

Introduction

Electrocaloric effect (ECE) is a change in the temperature and entropy of a material when an external electrical field is applied or removed under adiabatic conditions, and it may provide an efficient way to realize the solid-state cooling device [1], [2], [3], [4], [5], [6]. A lot of interest had been concentrated on the ECE of bulk ferroelectric materials in the 1960s and 1970s, but no commercial application has been exploited because of the small ECE [3], [7]. The research interest has been reactivated recently after discovering giant ECEs in thin-film PbZr0.95Ti0.05O3 and [P(VDF-TrFE)] copolymer [1], [2], and then numerous studies of ECEs on all kinds of materials have been conducted [8], [9], [10], [11]. One of most important parameter to characterize the ECE is EC temperature change, ΔT (in Kelvin). So far, the highest EC ΔT of 45.3 K has been obtained by a field-induced antiferroelectric to ferroelectric phase transition around room temperature in Pb0.8Ba0.2ZrO3 thin film [12], while only several Kelvin has been observed in the bulk materials. A new parameter, electrocaloric strength ΔTE, has been introduced in order to compare the ECEs of different materials in various electrical fields, and the ferroelectric oxides have superior EC performance in this manner [4], [13]. Although thin films have the advantage on the application in small solid-state cooling devices, the bulk materials are essential to the EC application in the middle and/or large scale devices, such as solid state refrigeration [4], [5]. However, the highest EC temperature change in bulk materials is low, and they cannot fulfill the requirement of the practical application in the solid state cooling device [14], [15]. Furthermore, all bulk materials with high EC temperature change contain lead ions, which are not desired in the practical application since they harm our environment. The EC temperature changes of lead-free bulk materials are very small, so it is a big challenge to achieve high EC temperature changes in the lead-free bulk materials.

According to the previous work [5], the ECEs of bulk materials are restricted by dielectric strengths, that is, the low dielectric strengths of bulk materials lead to the small EC temperature changes. Thus, the ECE can be improved by enhancing the dielectric strength in the bulk materials. Recently, our group has attained a high EC temperature change, 3.08 K, in the Mn-substituted Ba0.65Sr0.35TiO3 ceramics prepared by the spark plasma sintering (SPS) process at room temperature [16]. The dielectric strength of Ba0.65Sr0.35TiO3 ceramics can be improved from 40 kV cm−1 to 90 kV cm−1 by the spark plasma sintering process, and it can be enhanced further to 130 kV cm−1 by substituting part of titanium with manganese ions. As a result, the EC temperature changes of corresponding ceramics increase from 0.83 K to 2.10 K, and then 3.08 K. Although the high ECE has been achieved in the above ceramics, the correlation between structures, especially microstructures and electrocaloric effects is not clear.

In the present work, the detail phase constitutions, microstructures and electrocaloric properties of Ba0.7Sr0.3TiO3-based ceramics have been investigated, and the correlation between these parameters is tried to be revealed in the paper.

Section snippets

Experimental procedure

Ba0.7Sr0.3TiO3 (BST) and Ba0.7Sr0.3Ti0.997Mn0.003O3 (BSTM) powders were synthesized via the standard solid-state reaction method. Stoichiometric mixtures of SrCO3 (99.9%), BaCO3 (99.93%), TiO2 (99.5%) and/or MnO (99.5%) were milled for 24 h in anhydrous alcohol using zirconia balls media and calcined at 1150 °C or 1100 °C in air for 3 h to yield BST or BSTM powders, respectively. Then, the calcined powders were reground by hand in an agate mortar, placed into a graphite die, and sintered under a

Results and Discussions

Fig. 1 shows the SEM micrographs of polished and thermal-etched surfaces for three ceramics. Some pores are observed on the surfaces of conventionally sintered Ba0.7Sr0.3TiO3 (CS-BST) ceramics, while there is almost no pore for the spark plasma sintered Ba0.7Sr0.3TiO3 (SPS-BST) and Ba0.7Sr0.3Ti0.997Mn0.003O3 (SPS-BSTM) ceramics, indicating that the relative density of CS-BST ceramic is lower than those of the others. Actually, the relative density of CS-BST is about 97% of the theoretical

Conclusions

The densification process for Ba0.7Sr0.3TiO3 and Ba0.7Sr0.3Ti0.997Mn0.003O3 ceramics can be enhanced by the spark plasma sintering process, where the fine grain structures are obtained with the smaller ferroelectric domain sizes, and the diffuse phase transition behaviors are determined. The fully dense ceramics with fine grain and domain structures can significantly enhance the dielectric strength, and subsequently result in the significant improvement of electrocaloric effects. The dielectric

Acknowledgments

This work was supported by National Natural Science Foundation of China under Grant nos. 51272233, 51332006 and 51202215.

References (28)

  • T.M. Correia et al.

    Investigation of electrocaloric effect in a PbMg2/3Nb1/3O3-PbTiO3 relaxor thin film

    Appl. Phys. Lett.

    (2009)
  • S.G. Lu et al.

    Comparison of directly and indirectly measured electrocalaoric effect in relaxor ferroelectric polymers

    Appl. Phys. Lett.

    (2010)
  • B.L. Peng et al.

    A giant electrocaloric effect in nanoscale antiferroelectric and ferroelectric phases coexisting in a relaxor Pb0.8Ba0.2ZrO3 thin film at room temperature

    Adv. Funct. Matrer

    (2013)
  • X. Moya et al.

    Giant electrocaloric strength in single-crystal BaTiO3

    Adv. Mater.

    (2013)
  • Cited by (71)

    • Flexocaloric effect in ceramics

      2023, Flexoelectricity in Ceramics and their Application
    • Electrocaloric Ceramics

      2023, Encyclopedia of Materials: Electronics
    View all citing articles on Scopus
    View full text