聚芳醚酮在太阳能电池集流系统中的导体作用

A. Chebotareva, T. Kost, A. Lachinov, S. Salazkin, V. Shaposhnikova
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引用次数: 0

摘要

本文研究了几种高分子主链上含有芴基团的热塑性共聚物聚芳醚酮(co-PAEK)的热力学和电学性能。目前正在研究co - paek在具有透明导电氧化物(TCO)电极和多线接触网格的太阳能电池接触系统中的应用。聚合物薄膜用作导电粘合剂,在金属丝和TCO之间形成电接触。在1 atm的超压和co-PAEK的最大变形温度下,层压过程中形成导电触点,共聚物从初始介电状态切换到稳定的高导电状态。合成了芴基团(q)含量为5、10、15、20和25 mol.%的co - paek,分子量相同,粘度降低~0.38 dl/g。为了选择每个coPAEK的最佳接触系统形成温度,根据热-力学曲线确定了玻璃化转变温度(T g)和峰值应变温度(T d)。结果表明,随着q的增加,温度T g从162°增加到185°С, T d从203°增加到223°С。根据共聚物中氟基团的含量,测定了金属线/co-PAEK/TCO (ITO - In2O3:Sn)体系中涂有铟:锡(in:Sn)焊料的圆铜线和镀锡线的比接触电阻(ρС)。(In:Sn)焊丝的比接触电阻ρС变化范围为0.56 ~ 0.83 mΩ cm2,镀锡焊丝的比接触电阻变化范围为- 0.84 ~ 1.43 mΩ cm2, q = 5 mol %的co-PAEK在两种情况下均表现出最低的ρС。研究了超声喷雾热解法生长的ITO在硅衬底上的电阻率对导线/co-PAEK/ITO触点的ρC的影响。在5 ~ 85℃的温度范围内,研究了导线/co-PAEK/ITO接触电阻率的温度依赖性,得出了金属型依赖性的结论。根据接触面积的微观研究结果,确定了接触形成后线与ITO之间典型的最小co-PAEK层厚度在0.5 ~ 2.4 μm之间。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
POLYARYLENE ETHER KETONES AS A CONDUCTOR IN THE SOLAR CELL CURRENT COLLECTION SYSTEM
The paper investigates the thermomechanical and electrical properties of a number of thermoplastic copolymers poly(arylene ether ketones) (co-PAEK) containing fluorene groups in the main chain of the macromolecule. Co-PAEKs are being studied for the purpose of their use in the contact system of a solar cell with a transparent conductive oxide (TCO) electrode and a multiwire contact grid. Polymer films are used as conductive adhesives to form an electrical contact between metal wire and TCO. The formation of an electrically conductive contact occurs during lamination at an excess pressure of 1 atm and a temperature of maximum deformation of co-PAEK, while the copolymer switches from the initial dielectric to a stable highly conductive state. Co-PAEKs with the content of fluorene groups ( q ) 5, 10, 15, 20 and 25 mol.% are synthesized, having the same molecular weight and the reduced viscosity of ~0.38 dl/g. To select the optimal contact system formation temperature for each coPAEK, the glass transition temperature ( T g) and the peak strain temperature ( T d) were determined from thermo mechanical curves. It was found that with increasing q , the temperature T g increases from 162 to 185°С, and T d from 203 to 223°С. The specific contact resistances (ρС) in the metal wire/co-PAEK/TCO (ITO - In2O3:Sn) system were determined for a round copper wire coated with indium:tin (In:Sn) solder, as well as for tin-plated wire, depending on the content of fluorene groups in the copolymer. The specific contact resistance ρС for wire with (In:Sn) solder varies in the range of 0.56-0.83 mΩ cm2, for tin-plated wire - 0.84-1.43 mΩ cm2, and co-PAEK with q = 5 mol % showed the lowest ρС in both cases. The ρC of wire/co-PAEK/ITO contacts has been studied as a function of the resistivity of ITO grown by ultrasonic spray pyrolysis on silicon substrates. The temperature dependence of the resistivity of the wire/co-PAEK/ITO contact was studied in the temperature range of 5-85°C, and a conclusion was made about the metallic type of dependence. According to the results of microscopic studies of the contact area, the typical minimum co-PAEK layer thickness between the wire and ITO after the formation of the contact was determined, which is in the range of 0.5-2.4 μm.
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