Domain switching and microcracking during poling of lead zirconate titanate ceramics

1993 ◽  
Vol 145 (1) ◽  
pp. 271-281 ◽  
Author(s):  
E. C. Subbarao ◽  
V. Srikanth ◽  
W. Cao ◽  
L. E. Cross
2001 ◽  
Vol 84 (12) ◽  
pp. 2921-2929 ◽  
Author(s):  
Alexandre E. Glazounov ◽  
Hans Kungl ◽  
Jan-Thorsten Reszat ◽  
Michael J. Hoffmann ◽  
Arnd Kolleck ◽  
...  

2020 ◽  
Vol 2020 ◽  
pp. 1-12
Author(s):  
Sheng Cang ◽  
Jiankang Chen ◽  
Chunsheng Lu

In this paper, the electromechanical behavior of lead zirconate-titanate ceramics (P51) has been characterized and modeled. The variation of the energy dissipation and peak electrical displacement of the P51 ceramic has been investigated in details. The total strain of P51 under cyclical loading consists of elastic deformation (εije), immediate ferroelectric domain switching deformation (εijd), and time-dependent deformation (εijc). Thus, an expression for the energy dissipation of P51 can be theoretically derived. In addition, a practical method for calculating the dissipated energy has been proposed by integrating the curve of a hysteresis loop. The experimental results show that the peak electrical displacement and dissipated energy both decrease monotonously with the increase of the number of cycles. Furthermore, ferroelectric 90° domain switching was observed by X-ray diffraction (XRD) and the percentage of domain switching has been calculated by the variation of the peak intensity ratio of (002) to (200) at about 45 degrees. Then, grain debonding, crack, and crush were found around voids inside the specimen by using scanning electron microscope (SEM). It is indicated that switching of more capable-switch domains stimulates larger dissipated energy and a bigger peak electrical displacement at the initial cyclic loading. Finally, an exponential functional model has been proposed to simulate the peak evolution of electrical displacement based on the energy dissipation of P51 ceramics under cyclical load.


2010 ◽  
Vol 4 (3) ◽  
pp. 426-434 ◽  
Author(s):  
Mitsuhiro OKAYASU ◽  
Eriko SUGIYAMA ◽  
Kazuto SATO ◽  
Mamoru MIZUNO

2008 ◽  
Vol 91 (5) ◽  
pp. 1586-1590 ◽  
Author(s):  
Jacob L. Jones ◽  
Alain B. Kounga ◽  
Emil Aulbach ◽  
Torsten Granzow

2008 ◽  
Vol 56 (7) ◽  
pp. 1577-1587 ◽  
Author(s):  
Soodkhet Pojprapai (Imlao) ◽  
Jacob L. Jones ◽  
Andrew J. Studer ◽  
Jennifer Russell ◽  
Nagarajan Valanoor ◽  
...  

Author(s):  
M.L.A. Dass ◽  
T.A. Bielicki ◽  
G. Thomas ◽  
T. Yamamoto ◽  
K. Okazaki

Lead zirconate titanate, Pb(Zr,Ti)O3 (PZT), ceramics are ferroelectrics formed as solid solutions between ferroelectric PbTiO3 and ant iferroelectric PbZrO3. The subsolidus phase diagram is shown in figure 1. PZT transforms between the Ti-rich tetragonal (T) and the Zr-rich rhombohedral (R) phases at a composition which is nearly independent of temperature. This phenomenon is called morphotropism, and the boundary between the two phases is known as the morphotropic phase boundary (MPB). The excellent piezoelectric and dielectric properties occurring at this composition are believed to.be due to the coexistence of T and R phases, which results in easy poling (i.e. orientation of individual grain polarizations in the direction of an applied electric field). However, there is little direct proof of the coexistence of the two phases at the MPB, possibly because of the difficulty of distinguishing between them. In this investigation a CBD method was found which would successfully differentiate between the phases, and this was applied to confirm the coexistence of the two phases.


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