Abstract:(Ba, Ca)(Ti, Zr)O3 ceramics have been considered as a potential lead‐free alternative to commonly used lead‐based piezoelectric ceramics due to their high piezoelectric performance at room temperature. In this study, the bipolar fatigue behavior of this material is investigated at room temperature. Two compositions were cycled with a bipolar electric field signal at 10 Hz with a maximum of three times the coercive field for up to approximately 107 cycles. Both investigated compositions exhibited high bipolar f… Show more
“…The fatigue behavior of commercial soft PZT ceramics (e.g., PIC151) is also included for further comparison (Figure F) . Several studies previously published reported a very good fatigue resistance in KNN‐CZ5 and BCTZ ceramics (Figure F) . In the present work, a fatigue‐free behavior is obtained at x = 0.2, and that the fatigue resistance of the produced ceramics are either comparable to or better than the aforementioned ceramics.…”
Section: Resultssupporting
confidence: 61%
“… P ‐ E loops of the ceramics with (A) x = 0, (B) x = 0.2, (C) x = 0.5, (D) x = 0.8 after 10 0 and 10 6 cycles. Comparison of normalized P r of (E) ceramics with different La 3+ contents ( x = 0, 0.2, and 0.5) and (F) several representative lead‐free ceramics and PIC 151 ceramics [Color figure can be viewed at wileyonlinelibrary.com]…”
To improve the temperature stability and electrical properties of KNN‐based ceramics, we simultaneously consider the phase boundary and the addition of rare earth element (La), 0.96K0.5Na0.5Nb0.96Sb0.04O3‐0.04(Bi1‐xLax)0.5Na0.5ZrO3 (0 ≤ x ≤ 1.0) ceramics. More specifically, we investigate how the phase boundary and the addition of La3+ affect the phase structure, electrical properties, and temperature stability of the ceramic. We show that increasing the La3+ content leads to a change in phase structure, from a rhombohedral‐tetragonal (R‐T) phase coexistence to a cubic phase. More importantly, we show that the appropriate addition of La3+ (x = 0.2) can simultaneously improve the unipolar strain (from 0.127% to 0.147%) and the temperature stability (i.e., the unipolar strain of 0.147% remains unchanged when T is increased from 25 to 80°C). In addition, we find that the ceramics with x = 0.2 exhibit a large piezoelectric constant (d33) of ~430 pC/N, a high Curie temperature (TC) of ~240°C and a fatigue‐free behavior (after 106 electric cycles). The enhanced electrical properties mostly originate from the easy domain switching, whereas the improved temperature stability can be attributed to the R‐T phase boundary and the appropriate addition of La3+.
“…The fatigue behavior of commercial soft PZT ceramics (e.g., PIC151) is also included for further comparison (Figure F) . Several studies previously published reported a very good fatigue resistance in KNN‐CZ5 and BCTZ ceramics (Figure F) . In the present work, a fatigue‐free behavior is obtained at x = 0.2, and that the fatigue resistance of the produced ceramics are either comparable to or better than the aforementioned ceramics.…”
Section: Resultssupporting
confidence: 61%
“… P ‐ E loops of the ceramics with (A) x = 0, (B) x = 0.2, (C) x = 0.5, (D) x = 0.8 after 10 0 and 10 6 cycles. Comparison of normalized P r of (E) ceramics with different La 3+ contents ( x = 0, 0.2, and 0.5) and (F) several representative lead‐free ceramics and PIC 151 ceramics [Color figure can be viewed at wileyonlinelibrary.com]…”
To improve the temperature stability and electrical properties of KNN‐based ceramics, we simultaneously consider the phase boundary and the addition of rare earth element (La), 0.96K0.5Na0.5Nb0.96Sb0.04O3‐0.04(Bi1‐xLax)0.5Na0.5ZrO3 (0 ≤ x ≤ 1.0) ceramics. More specifically, we investigate how the phase boundary and the addition of La3+ affect the phase structure, electrical properties, and temperature stability of the ceramic. We show that increasing the La3+ content leads to a change in phase structure, from a rhombohedral‐tetragonal (R‐T) phase coexistence to a cubic phase. More importantly, we show that the appropriate addition of La3+ (x = 0.2) can simultaneously improve the unipolar strain (from 0.127% to 0.147%) and the temperature stability (i.e., the unipolar strain of 0.147% remains unchanged when T is increased from 25 to 80°C). In addition, we find that the ceramics with x = 0.2 exhibit a large piezoelectric constant (d33) of ~430 pC/N, a high Curie temperature (TC) of ~240°C and a fatigue‐free behavior (after 106 electric cycles). The enhanced electrical properties mostly originate from the easy domain switching, whereas the improved temperature stability can be attributed to the R‐T phase boundary and the appropriate addition of La3+.
“…[50][51][52] Development of these characterisation techniques and predictive modelling covering multiple length scales may be the key tools needed in order to design new reversible phase-change actuator ceramics with improved fatigue properties compared to present generation ceramics. 17,[53][54][55] The present study has shown that minimum grain-scale strain heterogeneity can be achieved by precise control of the lattice distortions of the resultant phases in the transformed state and that this in turn leads to the maximum achievable transformation strain. Designing materials to have controlled combinations of transformation symmetries and unit cell distortions may be challenging.…”
mentioning
confidence: 99%
“…From the above, it is obvious that the mixed phase volume fractions, as well as the average and width of the transformation strain distributions, are intimately linked to the rhombohedral and tetragonal lattice distortions. 55 (e r max ¼ 2.5%), while the tetragonal lattice distortion was modelled assuming the same pseudocubic unit cell a 0 ¼ 3.904 Å for the undistorted reference (initial state BNT-6.25BT, Table I), a constant volume of the distorted tetragonal unit cell (at field value for BNT-6.25BT), and c/a ratios varying in 25 steps between 1.000 (e t max ¼ 0.0%) and 1.038 (e t max ¼ 2.5%). All averages and widths of the transformation strain distributions are reported as fractions of the maximum achievable transformation strain for the particular combination of lattice parameters, thus either for a h111i-oriented rhombohedral or a h100i-oriented tetragonal grain.…”
Phase-change actuator ceramics directly couple electrical and mechanical energies through an electric-field-induced phase transformation. These materials are promising for the replacement of the most common electro-mechanical ceramic, lead zirconate titanate, which has environmental concerns. Here, we show that by compositional modification, we reduce the grain-scale heterogeneity of the electro-mechanical response by 40%. In the materials investigated, this leads to an increase in the achievable electric-field-induced strain of the bulk ceramic of 45%. Compositions of (100–x)Bi0.5Na0.5TiO3–(x)BaTiO3, which initially possess a pseudo-cubic symmetry, can be tuned to undergo phase transformations to combined lower symmetry phases, thus decreasing the anisotropy of the transformation strain. Further, modelling of transformation strains of individual grains shows that minimum grain-scale strain heterogeneity can be achieved by precise control of the lattice distortions and orientation distributions of the induced phases. The current results can be used to guide the design of next generation high-strain electro-mechanical ceramic actuator materials.
“…11,16 Though high strain memory is desired, its stability is more concerned. 12 It is noted that, compared with bipolar cycling, weaker fatigue effect happens under sesquipolar cycling supported by Yao et al 8 and Zhang et al, 18 which may be another reason for the enhanced stability of strain memory. Apparently, the evolution of strain memory vs cycle numbers depends significantly on E À .…”
The negative electric field, field cycling and frequency dependence of strain memory effect in poled and aged Mn‐doped Pb(Mn1/3Sb2/3)O3–Pb(Zr,Ti)O3 (PMS–PZT) piezoceramics under sesquipolar loading were investigated. The strain memory effect of Mn‐doped PMS–PZT is especially sensitive to the applied negative electric field. Maximum strain memory of 0.32% is achieved when the negative electric field is around negative coercive field of ~2.1 kV/mm, which can be ascribed to the partially depoled state with randomized domains. And this strain memory shows very good cycling stability, varying less than 5% up to 104 cycles, while almost 40% degradation is found under bipolar signal. In addition, due to the stabilized defect dipoles, the strain memory exhibits stable characteristic over a broad frequency range from 0.01 Hz to 20 Hz. The results may shed new insights into designing the novel strain memory actuators where stable strain state could be realized after the removal of electric field.
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