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Lead-based electro ceramics like PZT are the most commercially used as sensors, actuators and
transducers due to their excellent electromechanical response, however
The environmental concerns and the legislation imposed on hazardous materials, lead is considered
toxic and its use is banned for many applications. Therefore the alternative lead free electroceramics
have become the focus of research in both industry and academia. In our present work among the
several families of lead-free, we will focus on the bismuth-based ferroelectric ceramics due to their
excellent piezoelectric and ferroelectric properties.
In brief this thesis we will emphasize on the improvement of ferroelectric and field-induced strain
properties of BNKT-LS ceramic system by different alovilent and isovalent B-site substitutions.
The effect of zirconium (Zr+4), niobium (Nb+5) and tantalum (Ta+5) substitution for the B-site in the host
perovskite unit cell on the dielectric, electromechanical and piezoelectric properties of lead-free
0.99[Bi1/2(Na0.82K0.18)1/2TiO3]-0.01LiSbO3 (BNKT-LS) piezoceramics has been investigated. The ternary
BNKT-LS system was synthesized using low temperature conventional solid state reaction method.
Crystal structure, dielectric, ferroelectric and field-induced strain behavior of Zr modified lead-free
0.99[Bi1/2(Na0.82K0.18)1/2(Ti1-xZrx) O3]-0.01LiSbO3 (BNKTZ-LS) ceramics were investigated in composition
range x = 0 - 0.040. XRD patterns revealed the formation of pure perovskite phase with no apparent
structural phase transition with pseudo cubic symmetry for the compositions at low concentration of
dopants although there were some traces of secondary phases at higher concentrations. The
temperature-dependent dielectric peaks of the BNKTZ-LS ceramics broadened and ferroelectric
polarizations decreased with increasing Zr concentration. Ferroelectric and bipolar field induced-strain
curves indicated a disruption of ferroelectric order upon Zr addition into BNKT-LS ceramics. This
destabilization of the ferroelectric order was accompanied by an enhanced field-induced strain. A high
field-induced strain (S = 0.30%) with a normalized strain (d*33 = Smax/Emax = 500 pm/V) was observed at an
applied electric field of 6 kV/mm at x = 0.020. The Ta-modified 0.99[(Bi0.82Na18)TiO3-(Bi1/2K1/2)TiO3]-
0.01LiSbO3 (BNKTT-LS) piezoceramics were also synthesized by a conventional solid-state reaction
method. The effect of Ta addition into the BNKT-LS ceramics were studied through X-ray diffraction,
dielectric, temperature dependent ferroelectric and field-induced strain characterizations. As the Ta
content was increased, the maximum dielectric constant as well as the depolarization temperature (Td)
decreased. The polarization and strain hysteresis loops indicate that the addition of Ta significantly
disrupts the ferroelectric order of the BNKT-LS ceramics leading to a degradation of the remnant
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polarization and coercive field. However, the destabilization of the ferroelectric order is accompanied by
a significant enhancement in the unipolar strain. A large unipolar field-induced strain of 0.38% with a
normalized (d*33 = Smax/Emax = 650 pm/V) at a driving field of 6 kV/mm was obtained at room
temperature for x = 0.013. This significant strain enhancement is a result of the reversible phase
transition between a NP phase in a zero field and a field-induced ferroelectric phase. Finally the effect of
Nb-substitution on the dielectric, electromechanical and piezoelectric properties of Pb-free
0.99[Bi1/2(Na0.82K0.18)1/2Ti1-xNbxO3]-0.01LiSbO3 (BNKT-LS) piezoelectric ceramics has been investigated. X-
ray diffraction analysis reveals pseudo-cubic symmetry for the compositions with x = 0 - 0.030. Both the
dielectric constant εr and depolarization temperature Td decreased with an increase in Nb content. An
analysis of the electric field induced polarization and strain hysteresis loops indicated that Nb
substitution disrupted the long range ferroelectric order of BNKT-LS ceramics. This degraded the
remnant polarization, coercive field and piezoelectric coefficient d33 while the electric field induced
strain increased (peaked at x=0.015) to 0.43% corresponding to a normalized strain (d33* = 614 pm/V) at
a deriving field of 7 kV/mm. This abnormal strain enhancement may be attributed to the reversible
phase transition between the polar and non-polar phases. At high Nb concentrations, BNKNb-LS
ceramics shows a typical relaxor behavior.
So for all dopants the increase in concentration results in a decrease in the maximum dielectric
constant as well as the depolarization temperature Td, the disruption of the long range ferroelectric
order, the degradation of remnant polarization, coercive field and piezoelectric coefficient d33. This was
also accompanied by enhancement in the electric field induced strain.
This abnormal strain
enhancement could be attributed to a reversible phase transition between polar and non-polar phase
for all systems. For high doping level BNKT-LS ceramics showed a typical relaxor behaviour. |
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