Abstract
A RECTANGULAR frame pendulum (Herbert type), oscillating on a spherical glass bearing in contact with a metal surface and surrounded by an electrolytic solution, is known to exhibit a rate of damping which is roughly a parabolic function of the potential of the metal surface1 (cf. the classical electrocapillary curve). Rehbinder1 (see also Rozhanski2) envisaged the formation of “reversible micro-fissures” in the metal surface under deformation: the electrical double layer penetrated the orifice of the micro-fissure, reducing cohesion, and hence the hardness, of the metal.
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References
Rehbinder and Wenstrom, Acta Physicochim., 19, 36 (1944); Doklady Akad. Nauk., 68, 329 (1949).
Rozhanski, Zhurn. Tekn. Fis., 19, 1056 (1949).
Grahame, Technical Report, U.S. Office of Naval Research, 2, 19 (1950).
Frumkin and Gorodetskaya, Z. phys. Chem., 136, 215 (1928).
Gorodetskaya and Kabanov, Phys. Z. Sowjet., 5, 418 (1934).
Bockris and Azzam, Trans. Farad. Soc., 48, 145 (1952).
Karpachev and Stromberg, Acta Physicochim., 12, 523 (1940).
Barker, Dissertation, Cambridge (1947).
Bowden and Young, Research, 3, 235 (1950).
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BOCKRIS, J., PARRY-JONES, R. Determination of the Relative Electrode Potential of an Uncharged Metal in Solution. Nature 171, 930–931 (1953). https://doi.org/10.1038/171930a0
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DOI: https://doi.org/10.1038/171930a0
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