摘要Shock-induced phase transition of ferroelectric ceramic PZT 95/5 causes elastic stiffening and depolarization, releasing stored electrostatic energy into the load circuit. We develop a model to describe the response of the PZT ferroelectric ceramic and implement it into simulation codes. The model is based on the phenomenological theory of phase transition dynamics and takes into account the effects of the self-generated intensive electrical field and stress. Connected with the discharge model and external circuit, the whole transient process of PZT ceramic depoling can be investigated. The results show the finite transition velocity of the ferroelectric phase and the double wave structure caused by phase transition. Simulated currents are compared with the results from experiments with shock pressures varying from 0.4 to 2.8 GPa.
Abstract:Shock-induced phase transition of ferroelectric ceramic PZT 95/5 causes elastic stiffening and depolarization, releasing stored electrostatic energy into the load circuit. We develop a model to describe the response of the PZT ferroelectric ceramic and implement it into simulation codes. The model is based on the phenomenological theory of phase transition dynamics and takes into account the effects of the self-generated intensive electrical field and stress. Connected with the discharge model and external circuit, the whole transient process of PZT ceramic depoling can be investigated. The results show the finite transition velocity of the ferroelectric phase and the double wave structure caused by phase transition. Simulated currents are compared with the results from experiments with shock pressures varying from 0.4 to 2.8 GPa.
LAN Chao-Hui**;PENG Yu-Fei LONG Ji-Dong;WANG Qiang;WANG Wen-Dou
. Modeling of PZT Ferroelectric Ceramic Depolarization Driven by Shock Stress[J]. 中国物理快报, 2011, 28(8): 88301-088301.
LAN Chao-Hui**, PENG Yu-Fei LONG Ji-Dong, WANG Qiang, WANG Wen-Dou
. Modeling of PZT Ferroelectric Ceramic Depolarization Driven by Shock Stress. Chin. Phys. Lett., 2011, 28(8): 88301-088301.
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