非极性态多晶钛酸钡的能量损失

G. Marks, D. Skaar
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引用次数: 0

摘要

基于在示波器屏幕上观察到的利萨尤图,描述了测定电介质中,特别是在较高温度下的电能损失的两种方法。这些方法被用来测定非极性态钛酸钡陶瓷在150°-550°C温度范围和20 Hz50 kHz频率范围内的损耗。第一种方法是在60赫兹的固定频率和相对较高的场强下使用。发现在固定温度和变场强E下,每克每循环的微热量损失L由关系式L = a2e2 + a4E4给出,其中a 2和a4为常数。在低场强下,第二项可以忽略。系数a2和4a随着开尔文温度的倒数呈指数变化。使用第二种方法在相对较低的场强下测定损耗,从200°到400°C观察到界面极化,表现为指数e"随着频率的降低而急剧上升,并且在恒温下每个e"相对于f曲线都有一个弯曲。发现双层聚光镜的麦克斯韦-瓦格纳方程描述了当f的指数为0.89而不是1时的现象,此时计算值与观测值的一致性较好。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Energy Loss in Nonpolar State Polycrystalline Barium Titanate
Two procedures, based on the Lissajous figure as observed on the screen of an oscilloscope, are described for the determination of electrical energy loss in dielectrics, particularly at higher temperatures. These procedures were employed to determine the losses in nonpolar state ceramic barium titanate within the temperature region 150°-550°C and over the frequency range 20 Hz50 kHz. The first procedure was used at a fixed frequency of 60 Hz and at relatively high field strengths. It was found that the loss L in microcalories per gram per cycle at fixed temperature and variable field strength E is given by the relation L = a 2 E2 + a4E4 where a 2 and a 4 are constants. At low field strengths the second term can be neglected. Coefficients a 2 and a 4 vary exponentially with the reciprocal of the Kelvin temperature. Using the second procedure at comparatively low field strengths for loss determination, interfacial polarization was observed from 200° to 400°C as shown by a sharp rise in the index e" with decrease in frequency and by an inflection in each e" versus f curve at constant temperature. It was found that the Maxwell-Wagner equation for a two-layer condenser describes the phenomenon provided that the exponent of f is 0.89 rather than unity, the concordance between calculated and observed values of e" then being quite good.
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