Llovera-Segovia Pedro, Ortega-Braña Gustavo, Fuster-Roig Vicente, Quijano-López Alfredo
Instituto de Tecnología Eléctrica, Universitat Politècnica de València, Camino de Vera s/n, 46022 Valencia, Spain.
Instituto Tecnológico de la Energía (ITE), Carrer de Juan de la Cierva y Codorniu 24, Paterna, 46980 Valencia, Spain.
Polymers (Basel). 2021 Jan 21;13(3):333. doi: 10.3390/polym13030333.
Piezoelectric polymer cellular films have been developed and improved in the past decades. These piezoelectric materials are based on the polarization of the internal cells by means of induced discharges in the gas inside the cells. Internal discharges are driven by an external applied electric field. With this polarization method, cellular polypropylene (PP) polymers exhibit a high piezoelectric coefficient d and have been investigated because of their low dielectric polarization, high resistivity, and flexibility. Charging polymers foams is normally obtained by applying a corona discharge to the surface with a single tip electrode-plane arrangement or a triode electrode, which consists of a tip electrode-plane structure with a controlled potential intermediate mesh. Corona charging allows the surface potential of the sample to rise without breakdown or surface flashover. A charging method has been developed without corona discharge, and this has provided good results. In our work, a method has been developed to polarize polypropylene foams by applying an insulated high-voltage electrode on the surface of the sample. The dielectric layer in series with the sample allows for a high internal electric field to be reached in the sample but avoids dielectric breakdown of the sample. The distribution of the electric field between the sample and the dielectric barrier has been calculated. Experimental results with three different electrodes present good outcome in agreement with the calculations. High d constants of about 880 pC/N have been obtained. Mapping of the d constant on the surface has also been carried out showing good homogeneity on the area under the electrode.
在过去几十年中,压电聚合物多孔膜得到了发展和改进。这些压电材料基于通过多孔膜内气体中的感应放电使内部单元极化。内部放电由外部施加的电场驱动。采用这种极化方法,多孔聚丙烯(PP)聚合物表现出高压电系数d,并且由于其低介电极化、高电阻率和柔韧性而受到研究。给聚合物泡沫充电通常是通过使用单尖端电极-平面装置或三极管电极(由具有可控电位中间网的尖端电极-平面结构组成)对表面施加电晕放电来实现的。电晕充电可使样品的表面电位升高而不会发生击穿或表面闪络。已经开发出一种无电晕放电的充电方法,并且取得了良好的效果。在我们的工作中,开发了一种通过在样品表面施加绝缘高压电极来使聚丙烯泡沫极化的方法。与样品串联的介电层可使样品中达到高内部电场,但避免样品发生介电击穿。已经计算了样品与介电阻挡层之间的电场分布。使用三种不同电极的实验结果与计算结果一致,取得了良好的结果。获得了约880 pC/N的高d常数。还对电极下区域的d常数进行了表面映射,显示出良好的均匀性。