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Simulation of the electrical transient during the porous anodizing of pure aluminium substrate

机译:纯铝基材多孔阳极氧化过程中电气瞬态的仿真

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Electrical transients were recorded during the anodizing of highly pure aluminium in phosphoric electrolyte, carried out in potentiostatic mode (25-150V) or in galvanostatic conditions (20-1000A/m{sup}2). The experimental reproductibility is satisfactory, according to the low standard deviations. For the galvanostatic mode, the voltage experimental transients show a "bell shape", characterized by some significant parameters (S{sub}0, t{sub}m, V{sub}m, V{sub}(ss)). Two mathematical relations were then proposed to simulate the voltage transient curves considering two parts, i.e. before and after the maximum (V{sub}m, t{sub}m). The validity of these computational simulations was next checked by comparison with the corresponding experimental curves. All the corresponding fittings of voltage transients are in good agreement, especially for the first part of the experimental curves, within the current densities range. Then, these computational simulations were correlated with the corresponding experimental FEG-SEM plan-views. By analogy with the nucleation phenomena during the metal electrodeposition, the "bell shaped" curves could be interpreted by the initial formation of a highly resistive oxide layer, followed by the subsequent appearance of the nanopores. The pores formation was in part explained showing that the V{sub}m experimental values obtained with the galvanostatic mode are closed to the previous critical voltage value U{sub}c initializing the anodic dissolution phenomenon.
机译:在高纯铝中的磷电解质阳极氧化期间记录电瞬变,在肺电极模式(25-150V)或在Galvanostatic条件下进行(20-1000A / m {sup} 2)。根据低标准偏差,实验性繁殖是令人满意的。对于镀锌模式,电压实验瞬变显示出“钟形”,其特征在于一些显着参数(S {Sub} 0,T {Sub} M,V {Sub} M,V {Sub}(SS))。然后提出了两个数学关系来模拟考虑两个部分的电压瞬态曲线,即在最大(v {sub} M,T {sub} M)之前和之后。接下来通过与相应的实验曲线进行比较检查这些计算模拟的有效性。电压瞬态的所有相应配件都很吻合,特别是对于实验曲线的第一部分,在当前密度范围内。然后,这些计算模拟与相应的实验Feg-SEM计划视图相关。通过在金属电沉积期间与成核现象进行类比,“钟形”曲线可以通过高电阻氧化物层的初始形成来解释,然后进行纳米孔的随后外观。孔形成部分地说明,通过镀锌模式获得的V {Sub} M实验值被关闭到先前的临界电压值U {ub} C初始化阳极溶解现象。

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