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An analytical axisymmetric model for the poling-history dependent behavior of ferroelectric ceramics

机译:铁电陶瓷的极化历史相关行为的解析轴对称模型

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The poling-history dependent behavior of ferroelectric ceramics has been investigated by experimental tests. A suddenly poled ferroelectric ceramic was found to have significantly larger remnant polarization and strain than the corresponding values of a gradually poled one. To explain this phenomenon, a new domain-switching criterion for ferroelectric ceramics is proposed, in which each 180degrees switching is divided into two successive 90degrees switchings. In a suddenly poled ceramic, the strong intergranular interaction after the first 90degrees switching is favorable for accomplishing the second 90degrees switching. The effects of poling-dependent effects are then taken into account by evaluating different levels of energy dissipation after the first 90degrees switching. The domain orientation distribution function (ODF) as well as the macroscopic polarization and strain are analytically derived under cyclic electric loading. In the non-dissipation case, the macroscopic polarization of a ferroelectric ceramic can be ideally saturated as long as the magnitude of the applied electric field exceeds root2-E-C (E-C is the coercive field), while in the full dissipation case, the maximum macroscopic polarization is related to the magnitude of the applied electric field. The hysteresis loops for the non-dissipation case are almost identical to the corresponding loops of a suddenly poled ceramic, and the hysteresis loops for the full dissipation case are very close to those of a gradually poled ceramic. The good agreement between the analytical and experimental results indicates the validity of the proposed model in describing the poling-history dependent effects in ferroelectric ceramics.
机译:铁电陶瓷的极化历史依赖行为已通过实验测试进行了研究。发现突然极化的铁电陶瓷具有比逐渐极化的陶瓷的相应值大得多的剩余极化和应变。为了解释这种现象,提出了一种新的铁电陶瓷磁畴转换准则,其中将每个180度转换分为两个连续的90度转换。在突然极化的陶瓷中,第一个90度切换后的强晶间相互作用有利于完成第二个90度切换。然后,通过在第一个90度切换后评估不同级别的能量耗散,来考虑极化相关效应的影响。在循环电载荷作用下,解析得出了畴取向分布函数(ODF)以及宏观极化和应变。在非耗散情况下,只要所施加电场的大小超过root2-EC(EC为矫顽场),铁电陶瓷的宏观极化就可以理想地饱和,而在全耗散情况下,最大宏观极化与所施加电场的大小有关。非耗散情况下的磁滞回线几乎与突然极化陶瓷的相应回路相同,而全耗散情况下的磁滞回线与逐渐极化的陶瓷非常接近。分析结果与实验结果之间的良好一致性表明,该模型在描述铁电陶瓷的极化历史相关效应方面是有效的。

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