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Ion Distribution in Ionic Electroactive Polymer Actuators

机译:离子电活性聚合物致动器中的离子分布

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Ionic electroactive polymer (i-EAP) actuators with large strain and low operation voltage are extremely attractive for applications such as MEMS and smart materials and systems. In-depth understanding of the ion transport and storage under electrical stimulus is crucial for optimizing the actuator performance. In this study, we show the dominances of ion diffusion charge and we perform direct measurements of the steady state ion distribution in charged and frozen actuators by using Time-of-Flight Secondary Ion Mass Spectrometry (ToF-SIMS). High temperature actuators that consist Aquivion ionomer membrane and high melting temperature ionic liquid l-butyl-2,3-dimethylimidazolium chloride (BMMI-C1]) served in this study. Electrical impedance, I-V characteristics, and potential step charging of the actuator are characterized at 25°C and 100°C. The conductivity of the actuator is 0.3mS/cm at 100°C and 2.9uS/cm at 25°C, respectively. The electrochemical window of the device is 3 V and a 2mm tip displacement is observed under 2.5 V 0.2Hz at 100°C. A semi-quantitative depth profile of the relative ion concentration in charged and frozen actuators is measured by ToF-SIMS. The result shows that, unlike semiconductors, ions do not deplete from the electrodes with same signs. Due to a strong cluster effect between the ions, Cl- and BMMI+ accumulate near both cathode and anode. Furthermore, the profile indicates that the ion size difference causes the BMMI+ space charge layers (~6um) much thicker than those of Cl" (~0.5um).
机译:具有大应变和低工作电压的离子电活性聚合物(i-EAP)执行器对于MEMS和智能材料及系统等应用极为有吸引力。深入了解电刺激下的离子传输和存储对于优化执行器性能至关重要。在这项研究中,我们展示了离子扩散电荷的优势,我们使用飞行时间二次离子质谱(ToF-SIMS)对带电和冻结致动器中的稳态离子分布进行了直接测量。由Aquivion离聚物膜和高熔点离子液体1-丁基2,3-二甲基咪唑鎓氯化物(BMMI-C1])组成的高温执行器在本研究中发挥了作用。致动器的电阻抗,IV特性和电位阶跃充电的特征是在25°C和100°C时。执行器的电导率在100°C下为0.3mS / cm,在25°C下为2.9uS / cm。器件的电化学窗口为3 V,在100 V的2.5 V 0.2Hz下观察到2mm的针尖位移。通过ToF-SIMS测量带电和冻结致动器中相对离子浓度的半定量深度曲线。结果表明,与半导体不同,离子不会以相同的符号从电极中耗尽。由于离子之间的强簇效应,Cl-和BMMI +聚集在阴极和阳极附近。此外,该曲线表明,离子尺寸差异导致BMMI +空间电荷层(〜6um)比Cl“(〜0.5um)厚得多。

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