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首页> 外文期刊>The Journal of Chemical Physics >NONEQUILIBRIUM FLUCTUATION THEORY IN ELECTROCHEMICAL NUCLEATION .3. EXPERIMENTAL DETERMINATION OF FLUCTUATION GROWTH RATE IN SILVER NUCLEATION ONTO PLATINUM ELECTRODE
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NONEQUILIBRIUM FLUCTUATION THEORY IN ELECTROCHEMICAL NUCLEATION .3. EXPERIMENTAL DETERMINATION OF FLUCTUATION GROWTH RATE IN SILVER NUCLEATION ONTO PLATINUM ELECTRODE

机译:电化学成核中的非平衡波动理论.3。铂电极上银成核的波动增长率的实验测定

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Following part II, in this paper, some analytical equations concerning nucleation current were experimentally examined for silver nucleation onto platinum electrode in AgNO3 + NaNO3 solution. After passing the minimum state, the nonequilibrium fluctuations being to unstably grow, being accompanied with active nucleation. Resultant current can be theoretically expressed as an exponential function of the second order of time, and its time coefficient depends on the concentrations of both depositing metal ion and supporting electrolyte and also the overpotential. These theoretical predictions were experimentally ascertained. Accordingly, it was concluded that the nucleation current is described by the quantities with regard to the fluctuations and the double layer. Furthermore, the maximum peak current appearing after nucleation growth current was investigated. As discussed before, the semilog plot of the current against the overpotential gave almost the same slope of the Tafel equation for silver deposition. Observed values of the current were almost equal to those measured by applying current steps to silver electrode. Finally, the diffusion current was expected after passing the peak current. Then, it was clarified that limiting diffusion current, indifferent to the initial value of the overpotential, flows according to the Cottrel equation. (C) 1997 American Institute of Physics. [References: 9]
机译:在第二部分之后,本文通过实验研究了有关成核电流的一些解析方程,以研究银在AgNO3 + NaNO3溶液中在铂电极上成核的过程。通过最小状态后,不平衡波动将不稳定地增长,并伴随着主动形核。合成电流理论上可以表示为第二级时间的指数函数,其时间系数取决于沉积的金属离子和支持电解质的浓度以及过电势。这些理论预测是通过实验确定的。因此,可以得出结论,成核电流由关于波动和双层的量来描述。此外,研究了在成核生长电流之后出现的最大峰值电流。如前所述,电流对超电势的半对数图给出了与银沉积塔菲尔方程几乎相同的斜率。观察到的电流值几乎等于通过对银电极施加电流阶跃而测得的值。最终,在通过峰值电流之后可以期待扩散电流。然后,根据Cottrel方程式,对与过电势的初始值无关的极限扩散电流进行了澄清。 (C)1997美国物理研究所。 [参考:9]

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