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PIEZOEFFECT IN POLAR MATERIALS USING MOMENT THEORY

机译:基于矩理论的极性材料的压电效应

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摘要

A method for describing the piezoelectric effect in a polar material is proposed based on the use of a composite particle model with seven degrees of freedom and a nonzero dipole moment. Based on micropolar theory, a system of equations is obtained which differs from the classical theory of piezoelectricity in the presence of additional terms. It is shown that under certain assumptions, the proposed system of equations becomes the classical system but the piezoelectric moduli depend strongly on the spontaneous polarization vector. It is shown that for anisotropic media with different symmetries, the structure of the third-rank piezoelectric tensors obtained using the proposed micropolar theory coincides with the structure of the tensors obtained using classical theory. For the media considered, dispersion relations are given and it is shown that in the proposed theory, unlike classical theory, the piezoelectric moduli are proportional to the spontaneous polarization.
机译:基于具有七个自由度和非零偶极矩的复合粒子模型,提出了一种描述极性材料中压电效应的方法。基于微极理论,获得了一个方程系统,该方程系统在存在附加项的情况下不同于经典的压电理论。结果表明,在某些假设下,所提出的方程组成为经典系统,但压电模量强烈依赖于自发极化矢量。结果表明,对于具有不同对称性的各向异性介质,利用微极性理论获得的三阶压电张量的结构与利用经典理论获得的张量的结构一致。对于所考虑的介质,给出了色散关系,并且表明在所提出的理论中,与经典理论不同,压电模量与自发极化成比例。

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