聚苯乙烯-二氧化钛复合材料作为介质材料

D Khastgir, H.S Maiti , P.C Bandyopadhyay
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引用次数: 26

摘要

本文研究了金红石聚苯乙烯压块中环境介电效应随频率和组成的函数,探讨了其作为电子材料的可能性,并在现有理论的基础上对其进行了表征。这些体系明显背离了物理混合定律。各频率下,介电常数λ′和损耗λ″随二氧化钛含量的增加而增大;这两个参数随频率的增加而减小。随着频率的降低,界面极化的程度大大增加。致密密度所证明的非分散性在约60 wt. %二氧化钛时达到最大值,此时不同的颗粒最松散地相互配合,形成相当多孔的基质。在体积分数中,御′和(御′)−1都是曲线状的,但御′在重量混合图中显示出在50wt . %处的断裂,反映了相互作用模式和程度的变化。该系统符合克劳修斯-莫索蒂方程。这种情况介于分别可能的Böttcher-Bruggeman和麦克斯韦-瓦格纳模型之间。这是由于非极性环境的施加以及随之而来的电荷密度和长程和短程力的减少,偶极矩和ε′随着聚苯乙烯的增加而减少。样品制备技术的变化极大地改变了这些致密材料的介电性能。通过改变组合物和制备方法,可以制备具有广泛介电性能的复合材料。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Polystyrene-titania composite as a dielectric material

Ambient dielectric effects have been studied in rutile-polystyrene compacts as functions of frequency and composition to explore the possibility of their use as electronic materials and characterize them on the basis of existing theories. The systems reveal marked departures from the law of physical mixtures. The dielectric constant ϵ′ and loss ϵ″ increase with increasing titania content at each frequency; both parameters decrease with increasing frequency. The extent of interfacial polarization is substantially augmented as the frequency is reduced. Heterodispersity evidenced from compact densities is a maximum at around 60 wt. % titania where the dissimilar particles fit most loosely into one another forming fairly porous matrices. ϵ′ and (ϵ′)−1 are both curvilinear in the volume fraction, but ϵ′ shows a break at 50 wt. % in the gravimetric-blend plot, reflecting a change in the pattern and degree of interactions. The system conforms to the Clausius-Mossotti equation. The situation is intermediate between the separately possible Böttcher-Bruggeman and Maxwell-Wagner models. This is ascribed to the decrease of dipole moment and ϵ′ with increasing polystyrene owing to the imposition of non-polar environments and consequent lessening of charge density and long- and short-range forces. The variation in sample preparation technique greatly modifies the dielectric properties of these compacts. The composites with a wide range of dielectric properties can be prepared by changing the composition as well as the method of preparation.

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