Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power

Sergey I. Shkuratov; Evgueni F. Talantsev; Jason Baird; Henryk Temkin; Larry L. Altgilbers; Allen H. Stults

doi:10.1063/1.2263532

Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power

Sergey I. Shkuratov
, Evgueni F. Talantsev
, Jason Baird
, Henryk Temkin
, Larry L. Altgilbers
, Allen H. Stults

Mining and Explosives Engineering

Research output: Contribution to journal › Article › peer-review

Abstract

A poled lead zirconate titanate Pb(Zr52Ti48)O3 (PZT) polycrystalline piezoelectric ceramic energy-carrying element of a compact explosive-driven power generator was subjected to a longitudinal explosive shock wave (the wave front traveled along the polarization vector P0). The shock compression of the element at pressures of 1.5-3.8 GPa caused almost complete depolarization of the sample. Shock wave velocity in the PZT was determined to be 3.94 ± 0.27 km/s. The electric charge stored in a ferroelectric, due to its remnant polarization, is released during a short time interval and can be transformed into pulsed power. Compact explosive-driven power sources utilizing longitudinal shock wave depolarization of PZT elements of 0.35 to 3.3 cm3 volume are capable of producing pulses of high voltage, with amplitudes up to 22 kV, and up to 350 kW peak power.

Original language	American English
Journal	Proceedings of the 2005 Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter
DOIs	https://doi.org/10.1063/1.2263532
State	Published - Jan 1 2006

Keywords

Explosions
Ferroelectric Ceramics
High-Pressure Effects
Lead compounds
Piezoceramics
Shock Wave Effects
Titanium compounds
Zirconium

Disciplines

Explosives Engineering
Power and Energy

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10.1063/1.2263532License: Unspecified

Longitudinal Shock Wave Depolarization of Pb(Zr Ti )O PolycrysFinal published version, 305 KBLicense: Unspecified

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Shkuratov, S. I., Talantsev, E. F., Baird, J., Temkin, H., Altgilbers, L. L., & Stults, A. H. (2006). Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power. Proceedings of the 2005 Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter. https://doi.org/10.1063/1.2263532

Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power. / Shkuratov, Sergey I.; Talantsev, Evgueni F.; Baird, Jason et al.
In: Proceedings of the 2005 Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter, 01.01.2006.

Research output: Contribution to journal › Article › peer-review

Shkuratov, SI, Talantsev, EF, Baird, J, Temkin, H, Altgilbers, LL & Stults, AH 2006, 'Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power', Proceedings of the 2005 Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter. https://doi.org/10.1063/1.2263532

Shkuratov SI, Talantsev EF, Baird J, Temkin H, Altgilbers LL, Stults AH. Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power. Proceedings of the 2005 Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter. 2006 Jan 1. doi: 10.1063/1.2263532

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title = "Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power",

abstract = " A poled lead zirconate titanate Pb(Zr52Ti48)O3 (PZT) polycrystalline piezoelectric ceramic energy-carrying element of a compact explosive-driven power generator was subjected to a longitudinal explosive shock wave (the wave front traveled along the polarization vector P0). The shock compression of the element at pressures of 1.5-3.8 GPa caused almost complete depolarization of the sample. Shock wave velocity in the PZT was determined to be 3.94 ± 0.27 km/s. The electric charge stored in a ferroelectric, due to its remnant polarization, is released during a short time interval and can be transformed into pulsed power. Compact explosive-driven power sources utilizing longitudinal shock wave depolarization of PZT elements of 0.35 to 3.3 cm3 volume are capable of producing pulses of high voltage, with amplitudes up to 22 kV, and up to 350 kW peak power.",

keywords = "Explosions, Ferroelectric Ceramics, High-Pressure Effects, Lead compounds, Piezoceramics, Shock Wave Effects, Titanium compounds, Zirconium",

author = "Shkuratov, \{Sergey I.\} and Talantsev, \{Evgueni F.\} and Jason Baird and Henryk Temkin and Altgilbers, \{Larry L.\} and Stults, \{Allen H.\}",

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AU - Shkuratov, Sergey I.

AU - Talantsev, Evgueni F.

AU - Baird, Jason

AU - Temkin, Henryk

AU - Altgilbers, Larry L.

AU - Stults, Allen H.

PY - 2006/1/1

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N2 - A poled lead zirconate titanate Pb(Zr52Ti48)O3 (PZT) polycrystalline piezoelectric ceramic energy-carrying element of a compact explosive-driven power generator was subjected to a longitudinal explosive shock wave (the wave front traveled along the polarization vector P0). The shock compression of the element at pressures of 1.5-3.8 GPa caused almost complete depolarization of the sample. Shock wave velocity in the PZT was determined to be 3.94 ± 0.27 km/s. The electric charge stored in a ferroelectric, due to its remnant polarization, is released during a short time interval and can be transformed into pulsed power. Compact explosive-driven power sources utilizing longitudinal shock wave depolarization of PZT elements of 0.35 to 3.3 cm3 volume are capable of producing pulses of high voltage, with amplitudes up to 22 kV, and up to 350 kW peak power.

AB - A poled lead zirconate titanate Pb(Zr52Ti48)O3 (PZT) polycrystalline piezoelectric ceramic energy-carrying element of a compact explosive-driven power generator was subjected to a longitudinal explosive shock wave (the wave front traveled along the polarization vector P0). The shock compression of the element at pressures of 1.5-3.8 GPa caused almost complete depolarization of the sample. Shock wave velocity in the PZT was determined to be 3.94 ± 0.27 km/s. The electric charge stored in a ferroelectric, due to its remnant polarization, is released during a short time interval and can be transformed into pulsed power. Compact explosive-driven power sources utilizing longitudinal shock wave depolarization of PZT elements of 0.35 to 3.3 cm3 volume are capable of producing pulses of high voltage, with amplitudes up to 22 kV, and up to 350 kW peak power.

KW - Explosions

KW - Ferroelectric Ceramics

KW - High-Pressure Effects

KW - Lead compounds

KW - Piezoceramics

KW - Shock Wave Effects

KW - Titanium compounds

KW - Zirconium

UR - https://scholarsmine.mst.edu/min_nuceng_facwork/1188

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DO - 10.1063/1.2263532

M3 - Article

JO - Proceedings of the 2005 Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter

JF - Proceedings of the 2005 Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter

ER -

Longitudinal Shock Wave Depolarization of Pb(Zr₅₂Ti₄₈)O₃ Polycrystalline Ferroelectrics and Their Utilization in Explosive Pulsed Power

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