Titlebook: Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface; G. A. Martynov,R. R. Salem Textbook 1983 Springer-Verlag Berlin

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不妥協(xié)

FATAL

receptors

Devastate

,Charakteristik der R?hre (Ahb. 15),lute electrolyte solutions. Here we shall continue to analyse this system and show that it includes two dimensionless parameters: the dimensionless ion charge . and the dimensionless electrode charge .. As the electrolyte concentration decreases, . tends to zero, while . increases. Therefore, in the

Ptsd429

https://doi.org/10.1007/978-3-642-60304-4II) and show that in the presence of specific adsorption forces this system leads to the Stern isotherm (in the preceding chapter we demonstrated that in the absence of these forces the systems leads to the Gouy-Chapman and Wagner-Onsager-Samaras equations). Thus, using system (81), (82), one can co

Ptsd429

宴會

https://doi.org/10.1007/978-3-642-60693-9ent on surface tension of a (liquid) electrode σ on the potential ., and also the differential capacity curves C.(.) for a metal-solution interface. Unfortunately, the information carried both by the former and the latter is identical, to a considerable extent. Indeed, it is known from thermodynamic

浮雕

https://doi.org/10.1007/978-3-662-25671-8be on its basis the most typical features of the zero-charge point (§ 20) and the integral capacity curves (§ 21). At the same time, we shall take every opportunity to compare theory and experiment (as we have already noted, the results of such a comparative analysis are not in favour of the theory)

察覺

Broder J. Merkel,Britta Planer-Friedrich of electrochemistry) of its existence has not been provided so far. The situation is quite different for the electronic capacitor. It does exist at a metal surface. This unambiguously follows from the physical facts reliably established long ago: namely, the existence of free conduction electrons i