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Modified interphase theory to determine dielectric constant of particulate composite material at microwave frequency

机译:修正相间理论确定微波频率下颗粒复合材料的介电常数

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The permittivity of composites at 10 GHz is computed using various existing models like mixing law, power law (PL) and interphase power law (IPL). A deviation in permittivity values determined from the existing models with respect to the experimental values is observed, which gets more significant with increase in volume fraction (VF) of the inclusions. Interphase theory, has been modified to predict real part of permittivity of particulate-composite system. A simple linear model is predicted, where the inter phase layer is not considered to have fixed permittivity but varying - from permittivity values of filler (in vicinity to inclusions) to permittivity values of polymer where the interphase layer ends. The model is tested for alumina-polystyrene and titania-polystyrene composite system. XRD, SEM and optical micro graph studies show that the size of filler in the composite is less than that of probing wavelength and distribution of filler is sufficiently uniform in the matrix. The present model termed as, varying inter phase layer permittivity model (VIPLP) gives a very close result to the experimental values. Some inter esting facts that came out of the present model - (a) higher the permittivity difference between the filler and the polymer, the gradient of decrease in permittivity of interphase layer is rapid (b) with the increase in volume fraction of filler, the effective surface area of interaction increases, hence the permittivity of the interphase layer increases.
机译:使用各种现有模型(如混合定律,功率定律(PL)和相间功率定律(IPL))计算复合材料在10 GHz时的介电常数。观察到从现有模型确定的介电常数值相对于实验值的偏差,该偏差随着夹杂物的体积分数(VF)的增加而变得更大。相间理论已被修改,以预测颗粒复合系统介电常数的真实部分。预测了一个简单的线性模型,其中相间层不被认为具有固定的介电常数,而是变化的-从填料的介电常数值(在附近到夹杂物)到相间层终止处的聚合物的介电常数值。该模型针对氧化铝-聚苯乙烯和二氧化钛-聚苯乙烯复合体系进行了测试。 XRD,SEM和光学显微图研究表明,复合物中填料的尺寸小于探测波长,并且填料在基体中的分布足够均匀。被称为变化相间层介电常数模型(VIPLP)的本模型给出了与实验值非常接近的结果。从本模型中得出的一些有趣的事实-(a)填料和聚合物之间的介电常数差越高,相间层的介电常数下降的梯度越快(b)随着填料体积分数的增加,相互作用的有效表面积增加,因此相间层的介电常数增加。

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