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Diffusion of the hydrogen in nanocrystalline vanadium films

机译:氢在纳米晶钒薄膜中的扩散

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The beta -> alpha phase transition and diffusion of the hydrogen in nanocrystalline vanadium films were investigated. Films were deposited onto the glass substrate at the temperature 673 K and at room temperature. Transmission electron microscopy investigations of the structure of films showed that the averaged sizes of vanadium crystallites were 7 and 4 nm, respectively. The derivative of the electrical resistance of the saturated film revealed the broad beta -> alpha phase transition about 390 K. The diffusion coefficient of the hydrogen was obtained from the approximation of the time dependence of the increase of the electrical resistance of the non-saturated part of the film by an analytical expression. Values of the diffusion coefficient revealed the strong dependence on the concentration of the hydrogen. At small concentration of the hydrogen, the diffusion coefficient was equal to that in the bulk vanadium. At large concentrations of the hydrogen (above 20 at. %), the diffusion coefficient decreases by a thousand times. The activation energy of diffusion, calculated for samples with the large concentration of the hydrogen, is equal to (44.8 +/- 0.8) kJ/mol [(0.464 +/- 0.008) eV].
机译:β- >α相变和扩散氢在纳米晶体的钒的电影被调查。玻璃衬底温度673 K和室温。显微结构的调查影片显示,钒的平均大小纳米微晶是7岁和4岁。导数的电阻饱和电影揭示了广泛的β- >α相变约390 K。系数的获得氢近似的时间依赖性增加的电阻未饱和的一部分电影的分析表达式。揭示了强烈的依赖氢的浓度。扩散氢的浓度系数等于在散装钒。(以上20。减少一千倍。的能量扩散,计算出样本大浓度的氢,是相等的(44.8 + / - 0.8)焦每摩尔((0.464 + / - 0.008)eV)。

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