Enhancement of Electromechanical and Piezoelectric Charge Coefficient in Lead-Free Na<sub>0.2</sub>K<sub>0.3</sub>Bi<sub>0.5</sub>TiO<sub>3</sub> Ceramic through Poling Effect

In device applications like transportable gas ignitors, lighters, and energy storage, ferroelectric materials play a crucial role. When K<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1+</sup> is substituted into NBT ceramics (Na<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</inf>K<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.3</inf>Bi<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.5</inf>TiO<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</inf> or NKBT-30), the Effect of K<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1+</sup> on dielectric, electric field reliant (the poling field (E<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">P</inf>) from 10 to 52 kV/cm) piezoelectric coefficient (d<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">33</inf>), electromechanical coupling constant (k<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">p</inf>), properties were thoroughly investigated. The microstructural analysis highlighted that an optimal grain size distribution and phase purity are crucial for achieving superior piezoelectric performance. Our findings also revealed optimized poling parameters at E<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">P</inf> = 52 kV/cm, yielding an elevated piezoelectric coefficient of 100 pC/N and the electromechanical coupling factors of 0.43 (k<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">p</inf>) in NKBT with a high dielectric constant of ≈ 4000, a dielectric loss (tanδ) of 0.0299 in 100 kHz frequency. The impact of electric poling on the piezoelectric characteristics of Na<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</inf>K<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.3</inf>Bi<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.5</inf>TiO<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</inf> has been investigated across varying poling field strengths.

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Published
2024-09-22
DOI
https://doi.org/10.1109/uffc-js60046.2024.10793639
Primary Topic
Ferroelectric and Piezoelectric Materials
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article
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article

Enhancement of Electromechanical and Piezoelectric Charge Coefficient in Lead-Free Na0.2K0.3Bi0.5TiO3 Ceramic through Poling Effect

Saket Asthana, Ranjan Kumar Sahu
Ferroelectric and Piezoelectric Materials
article

Enhancement of Electromechanical and Piezoelectric Charge Coefficient in Lead-Free Na0.2K0.3Bi0.5TiO3 Ceramic through Poling Effect

Saket Asthana, Ranjan Kumar Sahu
article en

Abstract

In device applications like transportable gas ignitors, lighters, and energy storage, ferroelectric materials play a crucial role. When K<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1+</sup> is substituted into NBT ceramics (Na<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</inf>K<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.3</inf>Bi<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.5</inf>TiO<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</inf> or NKBT-30), the Effect of K<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1+</sup> on dielectric, electric field reliant (the poling field (E<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">P</inf>) from 10 to 52 kV/cm) piezoelectric coefficient (d<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">33</inf>), electromechanical coupling constant (k<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">p</inf>), properties were thoroughly investigated. The microstructural analysis highlighted that an optimal grain size distribution and phase purity are crucial for achieving superior piezoelectric performance. Our findings also revealed optimized poling parameters at E<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">P</inf> = 52 kV/cm, yielding an elevated piezoelectric coefficient of 100 pC/N and the electromechanical coupling factors of 0.43 (k<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">p</inf>) in NKBT with a high dielectric constant of ≈ 4000, a dielectric loss (tanδ) of 0.0299 in 100 kHz frequency. The impact of electric poling on the piezoelectric characteristics of Na<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</inf>K<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.3</inf>Bi<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.5</inf>TiO<inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</inf> has been investigated across varying poling field strengths.

Indian Institute of Technology Hyderabad (IN)
Openalex Percentile: Top 85%
Ferroelectric and Piezoelectric Materials
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