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Metal Gouy-Chapman diffuse-charge model

Some emphasis is given in the first two chapters to show that complex formation equilibria permit to predict quantitatively the extent of adsorption of H+, OH , of metal ions and ligands as a function of pH, solution variables and of surface characteristics. Although the surface chemistry of hydrous oxides is somewhat similar to that of reversible electrodes the charge development and sorption mechanism for oxides and other mineral surfaces are different. Charge development on hydrous oxides often results from coordinative interactions at the oxide surface. The surface coordinative model describes quantitatively how surface charge develops, and permits to incorporate the central features of the Electric Double Layer theory, above all the Gouy-Chapman diffuse double layer model. [Pg.7]

Fig. 1.10 Schematic view of the electrical double layer in agreement with the Gouy-Chapman-Stem-Grahame models. The metallic electrode has a negative net charge and the solvated cations define the inner limit of the diffuse later at the Helmholtz outer plane (OHP). There are anions adsorbed at the electrode which are located at the inner Helmholtz plane (IHP). The presence of such anions is stabilized by the corresponding images at the electrode in such a way that each adsorbed ion establishes the presence of a surface dipole at the interface... Fig. 1.10 Schematic view of the electrical double layer in agreement with the Gouy-Chapman-Stem-Grahame models. The metallic electrode has a negative net charge and the solvated cations define the inner limit of the diffuse later at the Helmholtz outer plane (OHP). There are anions adsorbed at the electrode which are located at the inner Helmholtz plane (IHP). The presence of such anions is stabilized by the corresponding images at the electrode in such a way that each adsorbed ion establishes the presence of a surface dipole at the interface...
Fig. 10.14 Schematic diagram of the double layer according to the Gouy-Chapman-Stern-Grahame model. The metal electrode has a net negative charge and solvated monatomic cations define the inner boundary of the diffuse layer at the outer Helmholtz plane (oHp). Fig. 10.14 Schematic diagram of the double layer according to the Gouy-Chapman-Stern-Grahame model. The metal electrode has a net negative charge and solvated monatomic cations define the inner boundary of the diffuse layer at the outer Helmholtz plane (oHp).
Fig. 6.64. The Gouy-Chapman model, (a) The excess charge density on the OHP is smaller in magnitude than the charge on the metal. The remaining charge is distributed in the solution. The diffuse charge region, (b), can be simulated by a sheath of charge gd placed at a distance k 1 from the x = 0 plane, as depicted in (c). Fig. 6.64. The Gouy-Chapman model, (a) The excess charge density on the OHP is smaller in magnitude than the charge on the metal. The remaining charge is distributed in the solution. The diffuse charge region, (b), can be simulated by a sheath of charge gd placed at a distance k 1 from the x = 0 plane, as depicted in (c).
The simplest model of the electrical double layer between a metal and an electrolyte is the simple capacitor visualized by Helmholtz as shown in Figure 14. The diffuse ion distribution in the liquid phase was recognized by Gouy and Chapman- to form a space charge region adjacent to the electrode surface. [Pg.19]


See other pages where Metal Gouy-Chapman diffuse-charge model is mentioned: [Pg.49]    [Pg.47]    [Pg.31]    [Pg.525]    [Pg.71]    [Pg.75]    [Pg.4]    [Pg.54]    [Pg.229]    [Pg.309]    [Pg.55]    [Pg.558]    [Pg.16]    [Pg.9]    [Pg.105]    [Pg.14]    [Pg.9]    [Pg.6]   
See also in sourсe #XX -- [ Pg.43 , Pg.45 , Pg.46 , Pg.47 , Pg.48 , Pg.49 , Pg.50 ]




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Chapman

Charge Model

Charge diffusive

Diffuse charges

Gouy-Chapman

Gouy-Chapman diffuse model

Gouy-Chapman diffuse-charge model

Gouy-Chapman model

Metallic charge

Model metallic

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