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Formation and structure of Ni-Ag layer by electrolytic deposition

机译:电解沉积Ni-Ag层的形成与结构

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Although nickel and silver have the same Bravais-lattice and the difference of atom radii is below 15%, the binary system Ni-Ag is generally immiscible in the solid state below 500℃ [1]. the reason for this is the positive energy of mixing (+22 kJ/mol [2]). In recent literature the formation of metastable solid solution of Ni-Ag is described [2-4]. the observed solid solution is produced by using PVD-, CVD-techniques, or mechanical alloying. i.e. techniques, which work far from the thermodynamic equilibrium. In the present work, the original aim was to deposit Ni and Ag electrolytically from the same solution as a crystal mixture with very fine grain size. Layers which consist of a ferromagnetic phase (Ni) and a diamagnetic phase (Ag) are very interesting iv view of special magnetic applications (i.e. giant magnetoresistance). The layer should consist mainly of a nickel phase and to a lesser extent part of a silver phase. Because of the large difference between the standard potentials of Ni and Ag, the authors used an electrolyte where the concentration of Ag ions is two orders of magnitude lower than the Ni ion concentration. At a strong negative polarization potential (high over-potential), this concentration of silver leads to a transport limited silver deposition and simultaneously to a charge transfer-controlled deposition of nickel. The high negative over-potential should result in a microstructure whit very fine gains. The relation of grain size and over-potential is well-known [5]. Therefore strong negative polarization potentials were chose in the following study. The electrolyte composition consisted of 0.7 mol/l NiSO_4, 0.002 mol/l AgNO_3 and 0.26 mol/l C_6H_5Na_3O_7. The pH-value of the solution was 5.5 and all depositions were carried out at room temperature (RT). The electrolyte based on the authors' own experience in the deposition of nickel layers with nanocrystalline microstructure [6] and was slightly modified. All potentials were measured against a Ag/AgCl-reference electrode.
机译:尽管镍和银具有相同的Bravais晶格且原子半径之差低于15%,但二元体系Ni-Ag通常在低于500℃的固态下不溶混[1]。原因是混合的正能量(+22 kJ / mol [2])。在最近的文献中描述了Ni-Ag的亚稳态固溶体的形成[2-4]。观察到的固溶体是通过使用PVD,CVD技术或机械合金化产生的。即远非热力学平衡的技术。在目前的工作中,最初的目的是从与晶粒尺寸非常细小的晶体混合物相同的溶液中电解沉积镍和银。从铁磁性相(Ni)和抗磁性相(Ag)组成的层是特殊磁性应用(即巨磁阻)的非常有趣的观点。该层应主要由镍相组成,并在较小程度上由银相组成。由于Ni和Ag的标准电势相差很大,因此作者使用了一种电解质,其中Ag离子的浓度比Ni离子的浓度低两个数量级。在强负极化电势(高过电势)下,这种银浓度会导致传输受限的银沉积,并同时导致电荷转移控制的镍沉积。高的负超电势将导致微结构获得非常好的增益。晶粒尺寸和超电势之间的关系是众所周知的[5]。因此,在下面的研究中选择了强的负极化电位。电解质组合物由0.7mol / l的NiSO_4、0.002mol / l的AgNO_3和0.26mol / l的C_6H_5Na_3O_7组成。溶液的pH值为5.5,所有沉积均在室温(RT)下进行。基于作者在具有纳米晶体微结构的镍层沉积中的经验[6],电解液进行了微调。相对于Ag / AgCl参比电极测量所有电势。

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