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Single-crystal surfaces double-layer capacity

Experiments show that the values for the double layer capacity at single crystal metal surfaces depend on the nature of the metal. This indicates that the metal surface cannot be considered as a perfect conductor, as was done in classical theories. It is well known that an overspill of metal electrons can occur at the boundary of a metal with vacuum. A similar overspill expected at a metal-solution interface would alter the double layer capacity by an amount depending on the type of metal. Models have been constructed in which the metal is represented by an electronic plasma in a uniformly, positively charged background, which is known as the jellium model [81,82]. The inclusion of the electron overspill into the integral equation theories of the electric double layer has been performed basically with the HAB model. [Pg.629]

Naneva and Popov et al. [4, 5] have studied Cd(OOOl) grown electrolytically in a Teflon capillary in NaF aqueous solution. A value of fpzc equal to —0.99 V (versus saturated calomel electrode (SCE)) was evaluated from minimum potential (Amin) on the differential capacity C-E curves obtained in dilute electrolyte. The zero charge potential was found to be practically independent of the crystallographic orientation. The Apzc and the irmer layer capacity of Cd(OOOl) single crystals were determined in KF solution as a function of temperature [5]. The positive values of AApzc/AT indicated that the water dipoles in the inner part of the double layer were orientated with their negative part to the electrode surface. It was found that the hydrophilicity of the electrodes was increasing in the order Cd(OOOl) < Ag(100)[Pg.768]

Surface and Double-layer Properties Valette [19] has analyzed earlier experimental data on the inner-layer capacity at PZC for Ag(lll), Ag(lOO), and Ag(llO) surfaces in order to estimate the surface area and capacitance contributions of superficial defects for real electrodes, as compared to ideal faces. Considering the application of surface spectroscopy techniques to single-crystal Ag electrodes, one should note that anisotropy of the SHG response for metal electrode allows one to analyze and correlate its pattern with interfacial symmetries and its variations by changing nonlinear susceptibility and the surface structure. Early studies on Ag(lll) single-crystal electrodes have... [Pg.918]

The differences between various Ag surfaces can be distinguished by comparing their surface morphology (generally, the surface of (110) crystal is more folded than that of (111)) and other properties, such as the surface density of atoms, the PZC, and double-layer capacitance. The double-layer properties of single-crystal Ag electrodes have been studied very intensively [3, 22-27]. Selected characteristics of various Ag surfaces are compared in Table 1, which shows that the higher the surface density of atoms, the more positive PZC becomes. Furthermore, Fig. 2 exemplifies differential capacity data of those Ag surfaces. [Pg.918]


See other pages where Single-crystal surfaces double-layer capacity is mentioned: [Pg.134]    [Pg.155]   
See also in sourсe #XX -- [ Pg.46 ]




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Double layer capacity

Double-crystal

Layered crystals

Layered surfaces

Single crystal surfaces

Single layer

Single-surface

Surface double layer

Surface layers

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