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Interface reversible

Another problem that is common for all membrane-based solid-state sensors is the ill-defined membrane-metal interface. A large exchange current density is required to produce a reversible interface for a stable potentiometric sensor response. One approach to improving this interface is to use conducting polymers. Conducting polymers are electroactive n-conjugated polymers with mixed ionic and electronic conductivity. They... [Pg.304]

A polarizable Interface is represented by a (polarizable) electrode where a potential difference across the double layer is applied externally, i.e., by applying between the electrode and a reference electrode using a potentiostat. At a reversible interface the change in electrostatic potential across the double layer results from a chemical interaction of solutes (potential determining species) with the solid. The characteristics of the two types of double layers are very similar and they differ primarily in the manner in which the potential difference across the interface is established. [Pg.148]

A comparison with the reversible interface can be made. The reversible solid electrolyte interface can be used in a similar way to explore the distribution of charge components at solid-water interfaces. As we have seen, the surface charge density, o, (Eqs. (3.1) and (iii) in Example 2.1) can be readily determined experimentally (e.g., from an alkalimetric titration curve). The Lippmann equations can be used as with the polarized electrodes to obtain the differential capacity from... [Pg.150]

For a reversible interface, such as Agl/aqueous solution, the electrostatic potential in the solution just outside the surface referred to zero at regions of solution infinitely remote from colloidal particles, the Volta potential, is calculated from the Nernst equation, the concentration of potential determining ions, and the zero-point-of-charge which is not usually the stoichiometric equivalence point. [Pg.154]

The characteristics of the diffuse electric double layer at a completely polarized interface, such as at a mercury/aqueous electrolyte solution interface are essentially identical with those found at the reversible interface. With the polarizable interface the potential difference is applied by the experimenter, and, together with the electrolyte, specifically adsorbed as well as located in the diffuse double layer, results in a measurable change in interfacial tension and a measurable capacity. [Pg.154]

Relaxed interfaces cannot be polarized unless special precautions are taken. Capacitances can of course be obtained as derived quantities by differentiating the surface charge with respect to the surface potentieil if changes In the latter are known, which is possible if the Nemst equation applies. We now discuss direct capacitance measurements on reversible interfaces. To start with, the response of such an interface to an applied field has to be considered. The basic problem is that not only are double layers built up, but also charge transfer across the interfaces takes place and diffusion of charge-determining ions to or from the surface starts to play a role. With regard to these physical processes only the sum-effect is measured, and this sum has to be divided into its parts to obtain the capacitance. Distinctions can be made because the three constituents mentioned react in a different way to the frequency of the external field. [Pg.335]

On the basis that the model introduced to obtain expressions for the kinetics of the forward and reverse interface reactions at equilibrium is also valid when an overpotential exists, the polarized potential given by Eq 3.34 replaces the equilibrium potential in the exponential term. For the oxidation component of the reaction, Eq 3.14 becomes ... [Pg.100]

An example of a polarizable interface is that between a mereury electrode and liquid water, since the concentration of mercury ions in the aqueous phase is quite negligible. In this case, it is common to assume a a practical convention that equilibrium at the interface exists when the emf of the mercury electrode-reference electrode pair vanishes, since a Galvani potential difference between mercury and water cannot be measured. An example of a reversible interface is that between a hydrous oxide solid and liquid water. In this case, and OH ions can cross the interface freely and are potential-determining. Equilibrium at the interface is established when the net ion transport across the interface vanishes, i.e., when there is no change in the pH value of the aqueous phase. Note that the interface between a soil particle and the soil solution is in general reversible. Any charged species that is adsorbed by the particle and found in the soil solution is potential-determining. [Pg.93]

We have seen how the adhesion of coatings and films varies remarkably with the elasticity, geometry and loading condition of the test method. However, it is also essential to understand how the delaminating crack can be inhibited by various mechanisms which amplify the adhesion to give adhesion energies up to 100,000 J m 2, far higher than the thermodynamic values of 0. t-10 J m 2 known to apply to smooth reversible interfaces. [Pg.347]

In the electrochemical literature it is useful to refer to a reversible interface or interfacial reaction as one whose potential is determined only by the thermodynamic potentials of the various electroactive species at the electrode surface. In other words, it is only necessary to take into account mass transport to and from the interface, and not the inherent heterogeneous kinetics of the interfacial reaction itself, when discussing the rate of the charge transfer reaction. This nomenclature has two principal disadvantages. First, it neglects the fact that mass transport to the interface, whether migration or diffusion, is inherently an irreversible or dissipative... [Pg.62]

Cells of the Nernst and Haber type constitute two extreme cases of Hquid cells with a reversible interface of immiscible electrolyte solutions. Intermediate cases are, however, common e.g. in analytical appUcations, ion-selective systems with non-ideal (lower than 100%) selectivity are used. [Pg.83]


See other pages where Interface reversible is mentioned: [Pg.574]    [Pg.153]    [Pg.40]    [Pg.140]    [Pg.326]    [Pg.115]    [Pg.381]    [Pg.780]    [Pg.662]    [Pg.93]    [Pg.1695]    [Pg.126]    [Pg.166]   
See also in sourсe #XX -- [ Pg.91 ]




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Interfaces Reversible with Respect to Single Ions

Reversible and Irreversible Interfaces

Reversible changes, interface properties

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