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首页> 外文期刊>The Journal of Chemical Physics >NONEQUILIBRIUM FLUCTUATION THEORY ON PITTING DISSOLUTION .3. EXPERIMENTAL EXAMINATIONS ON CRITICAL FLUCTUATION AND ITS GROWTH PROCESS IN NICKEL DISSOLUTION
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NONEQUILIBRIUM FLUCTUATION THEORY ON PITTING DISSOLUTION .3. EXPERIMENTAL EXAMINATIONS ON CRITICAL FLUCTUATION AND ITS GROWTH PROCESS IN NICKEL DISSOLUTION

机译:点蚀溶解的非平衡波动理论.3。镍溶解过程中临界波动及其增长过程的实验研究

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Following part II, current-time transient in nickel pitting dissolution has been examined. After the passive film is broken, the resultant diffusion current decreases to the minimum value. The: minimum current, as shown in part I, gives the ratio of the average critical concentration fluctuation on the completely active surface to its autocorrelation distance. Therefore, using the experimental data of the minimum current mentioned above and the average concentration fluctuation obtained in part II, the critical autocorrelation distance has been calculated. Since, in the stable region, the fluctuation is suppressed to maintain that the electrode surface is flat and stable, the autocorrelation distance tends to approach infinity. Therefore, the distance at the critical state is expected to be extraordinarily large; the value of about 1 mm has been actually obtained. This value is regarded to have some generality independent of the characteristics of the reaction because it is purely determined by the thermal motion of the solution particles. In fact, it is approximately agreeable with the value obtained for silver nucleation. Then, the fluctuations start unstable growth. As shown in part I, reflecting the fact that the instability arises from the electrostatic interaction of the solution particles in the electric double layer, the growth current substantially depends on the concentration of the supporting electrolyte and the externally applied electrode potential. (C) 1997 American Institute of Physics. [References: 11]
机译:在第二部分之后,已经检查了镍点蚀溶解中的当前时间瞬变。在无源膜破裂之后,所得的扩散电流减小到最小值。如第一部分所示,最小电流给出了完全活动表面上的平均临界浓度波动与其自相关距离的比率。因此,使用上述最小电流的实验数据和第二部分中获得的平均浓度波动,已计算出临界自相关距离。由于在稳定区域中抑制波动以保持电极表面平坦且稳定,所以自相关距离趋于接近无穷大。因此,在临界状态下的距离预计将非常大。实际上已经获得了大约1毫米的值。该值被认为具有与反应特性无关的一般性,因为它完全由溶液颗粒的热运动确定。实际上,其与银成核所获得的值大致吻合。然后,波动开始不稳定的增长。如第一部分所示,反映出不稳定性是由双电层中的溶液颗粒的静电相互作用引起的事实,生长电流基本上取决于支持电解质的浓度和外部施加的电极电势。 (C)1997美国物理研究所。 [参考:11]

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