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Confinement-Induced High Field Antiferroelectric-Like Behavior in a Poly(vinylidene fluoride-co- trifluoroethylene-co- chlorotrifluoroethylene)-graft-Polystyrene Graft Copolymer

机译:聚(偏二氟乙烯 - 共氟乙烯 - 共氯二氟乙烯) - 移植 - 聚苯乙烯接枝共聚物中的限制诱导的高场抗废料等行为

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Ferroelectric polymers based on poly(vinylidene fluoride) (PVDF) and its copolymers appears to be a choice for electric energy storage because of their relatively high permittivity (10-20) and high dc breakdown strength (ca. 700 MV/m for a test area of 2 cm2 ). By modifying PVDF with bulky comonomers such as chlorotrifluoroethylene (CTFE) and hexafluoropropylene (HFP), P(VDF-CTFE) and P(VDF-HFP) random copolymers recently have achieved a discharged energy density as high as 17-25 J/cm~3 at ~600 MV/m for millisecond discharge. Nevertheless, ferroelectric polymers have relatively high losses due to the delayed dipole switching with respect to the alternating electric field. For example, the typical dielectric loss at low fields, tanδ, for PVDF and its copolymers is about 0.02, substantially higher than that of the current state-of-the-art capacitor film, biaxially stretched polypropylene (BOPP, tanδ ~ 0.0002). At high electric fields, depending on the polymorphism (β- vs. α-crystals), their ferroelectric losses can be as high as 40-80% because of the ferroelectric hysteresis loops during switching (see Scheme 1A). This ferroelectric loss is also discharge time dependent; an additional 40% loss in discharged energy density when the discharge time decreases from 1 ms to 1 μs.
机译:基于聚(偏二乙烯乙烯)(PVDF)的铁电聚合物及其共聚物似乎是电能储存的选择,因为它们相对高的介电常数(10-20)和高直流击穿强度(约700mV / m进行测试面积2厘米)。通过用氯丁二乙烯(CTFE)和六氟丙烯(HFP)如氯丁二乙烯(CTFE)和六氟丙烯(HFP),P(VDF-CTFE)和P(VDF-HFP)随机共聚物最近达到17-25J / cm的排出能量密度来改变PVDF。 3在毫秒放电〜600 mV / m。然而,由于相对于交变电场的延迟偶极开关,铁电聚合物具有相对高的损耗。例如,对于PVDF的低场,Tanδ的典型介电损耗为约0.02,基本上高于当前最先进的电容膜,双轴拉伸聚丙烯(BOPP,Tanδ〜0.0002)的约0.02。在高电场,取决于多态性(β-α-晶体),由于切换期间铁电磁滞回路(参见方案1a),它们的铁电损耗可以高达40-80%。这种铁电损耗也依赖于排出时间;当放电时间从1ms降至1μs时,放电时间的额外40%的损耗。

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