1976
DOI: 10.1016/0022-5088(76)90037-0
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Electrochemical methods for studying diffusion, permeation and solubility of hydrogen in metals

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Cited by 286 publications
(109 citation statements)
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“…It will be interesting to examine the peculiarity of area and its influence on delayed fracture, for instance, heavy industrial region where air pollution level is high or coastal area in tropical region. 58,71) Electrochemical hydrogen permeation is an useful method to investigate hydrogen entry and diffusion in metals, [72][73][74][75][76][77][78][79][80][81] hydrogen traps, 81,82) and the method has been used to monitor hydrogen entry under outdoor exposure 34,38,83) and CCT 84) conditions. Omura et al have reported the correspondence between hydrogen permeation current at an exposure site and fracture ratio of exposure bolts.…”
Section: Ssrt After Outdoor Exposurementioning
confidence: 99%
“…It will be interesting to examine the peculiarity of area and its influence on delayed fracture, for instance, heavy industrial region where air pollution level is high or coastal area in tropical region. 58,71) Electrochemical hydrogen permeation is an useful method to investigate hydrogen entry and diffusion in metals, [72][73][74][75][76][77][78][79][80][81] hydrogen traps, 81,82) and the method has been used to monitor hydrogen entry under outdoor exposure 34,38,83) and CCT 84) conditions. Omura et al have reported the correspondence between hydrogen permeation current at an exposure site and fracture ratio of exposure bolts.…”
Section: Ssrt After Outdoor Exposurementioning
confidence: 99%
“…A temperatura foi mantida constante a 25°C. A partir das curvas experimentais de permeação foi calculado o coeficiente de difusão aparente de hidrogênio (Dapp) usando o método do tempo tangente (breakthrough time) [14]. ) e foi selecionada com o intuito de permitir a interação entre o material e o hidrogênio preso durante a deformação causada pelo ensaio de CTOD.…”
Section: Materiais E Métodosunclassified
“…The computational time step is set to ∆t = 5.0 × 10 −6 s and 1.0 × 10 −6 s in Case I and II, respectively. In both cases, the simulations are terminated at t max = 1.0 s. In order to compare with the experimental measurements, the hydrogen atomic fractions at film surface are converted into electric current using the relation (Boes and Züchner, 1976) 32) where I(t) denotes electric current at film surface, N A denotes the Avogadro constant, F denotes the Faraday constant, S = 1.2 cm 2 is surface area, and h (111) = ( √ 3/3)a H is the lattice spacing of (111) planes. A comparison of I(t) predicted by the simulations and the corresponding experimental data is shown in Fig.…”
Section: Model Validation For Hydrogen Desorption In Pd(111) Thin Filmsmentioning
confidence: 99%