Leadless piezoelectric ceramics
A lead-free piezoelectric and ceramic technology, applied in the field of piezoelectric ceramics, can solve problems such as the temperature limit of BNT application, and achieve the effects of increasing depolarization temperature, good high-temperature ferroelectricity, and low raw material cost
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Embodiment 1
[0021] For formula (1-x) Bi 0.5 Na 0.5 TiO 3 -xBi 0.8 La 0.2 FeO 3 , x=0.0125.
[0022] performance:
[0023] piezoelectric coefficient
Embodiment 2
[0025] For formula (1-x) Bi 0.5 Na 0.5 TiO 3 -xBi 0.8 La 0.2 FeO 3 , x=0.0375.
[0026] performance:
[0027] piezoelectric coefficient
Embodiment 3
[0029] For formula (1-x) Bi 0.5 Na 0.5 TiO 3 -xBi 0.8 La 0.2 FeO 3 , x=0.0625.
[0030] performance:
[0031] piezoelectric coefficient
d 33 (pC / N)
Coefficient k p
depolarization temperature
T d (℃)
(μC / cm 2 )
remanent polarization P r
(μC / cm 2 )
coercive field E c
(kV / mm)
X=0.0625
20
0.027
171
28
11
5.5
[0032] figure 1 is (1-x) Bi 0.5 Na 0.5 TiO 3 -xBi 0.8 La 0.2 FeO 3 (Where 0.0125≤x≤0.0625) The X-ray diffraction spectrum (XRD) of ceramics, it shows that the sample prepared under this condition is a single phase without other impurity phases. And, from the XRD spectra of these ceramics, it can be obtained that when x=0.0125, the ceramics have a trigonal-orthorhombic quasi-isomorphic phase boundary structure.
[0033] Figure 2a , 2b is (1-x) Bi 0.5Na 0.5 TiO 3 -xBi 0.8 La 0.2 FeO 3 (where 0.01...
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