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Equilibrated metal surface

Redox proteins do not usually equilibrate with a platinum metal surface and, therefore, in order to establish thermodynamic equilibrium one must add a mixture of redox mediators to the solution. These are the same strongly coloured organic dyes... [Pg.102]

A certain amount of work has been done to compare results obtainable with Ni and with other metals. This work concerned in particular the thermodynamics of the adsorption of H2 and the relative activities of the various metals for the equilibration of H2 and D2 and the hydrogenation of ethylene and benzene. In order to avoid the difficulties of partial inaccessibility of the metal surface, only impregnation catalysts were used. [Pg.306]

An important parameter is the time allowed for the adsorption steps. In principle, adsorption on a clean metal surface should be very rapid at ambient temperature. However, in practice, particularly with metals such as Fe, Co or Ni, there is often a substantial contribution from a slow adsorption process. An arbitrary time for approximate equilibration is normally determined by experimentation, e.g., by ascertaining the time after which the pressure in a volumetric system decreases at a rate less than a preset value. Typical adsorption times for Pt metals range from a few minutes... [Pg.554]

SAIE corrosion protection emphasizes the fact that the corrosion protection of a metal depends on the overall corrosion protective behavior of an entire system. If a plasma polymerization coating is changed, all factors must be optimized to yield the best result that can be attributed to the change. The essence of interface engineering lies in the tailoring of surfaces to facilitate the equilibration of surface states of different materials. [Pg.5]

Figure 16. Surface structure the (0001) surface of sapphire (a-A Os) from Eng et al. (2000) with permission of the editor of Science, (a) Structure of vacuum-equihbrated diy surface. Al metal atoms sit on the surface, (b) Ideal bulk terminated surface with no relaxation or reconstraction. (c) Model for the wet-equihbrated surface at one atmosphere from surface scattering (ciystal truncation rod) diffraction measurements. Al metal atoms have shifted, the surface is oxygen terminated, and an organized water monolayer is required to accurately describe the observations, (d) Structure of gibbsite or y-Al(OH)3. The relaxed wet-equilibrated sapphire surface is intermediate between this structure and that of the bulk terminated stracture (B). Figure 16. Surface structure the (0001) surface of sapphire (a-A Os) from Eng et al. (2000) with permission of the editor of Science, (a) Structure of vacuum-equihbrated diy surface. Al metal atoms sit on the surface, (b) Ideal bulk terminated surface with no relaxation or reconstraction. (c) Model for the wet-equihbrated surface at one atmosphere from surface scattering (ciystal truncation rod) diffraction measurements. Al metal atoms have shifted, the surface is oxygen terminated, and an organized water monolayer is required to accurately describe the observations, (d) Structure of gibbsite or y-Al(OH)3. The relaxed wet-equilibrated sapphire surface is intermediate between this structure and that of the bulk terminated stracture (B).
All metal amination catalysts are active in the disproportionation of amines, which can lead to equilibration of primary, secondary, and tertiary amines. For example, for simple primary amines the initial step is the formation of an aldimine by dehydrogenation (Scheme 2). Subsequent addition of an amine and hydrogenation lead to a mixture of primary, secondary, and tertiary amines. The same active metal sites catalyze alcohol amination and amine disproportionation, which explains why the reactant alcohol inhibits disproportionation and selectivity for the desired amine drops considerably only after consumption of alcohol [2]. It is also evident from Scheme 2 that sufficient hydrogen present on the metal surface can reduce the concentration of imine and thus suppress disproportionation. [Pg.249]

Some experiments very similar to these outlined above were carried out by Ruch and Bartell [31]. Metal surfaces were equilibrated with aqueous decylamine, and the air-liquid-solid contact angles were then measured, using small air bubbles. The degree of adsorption of the decylamine was determined by optical measurements of the thickness of the film, but could be only approximately related to actual amounts adsorbed. While the results correlated well with a semi-empirical analysis, they unfortunately do not allow a verification of Equation 25. As shown in Figure 5, a qualitative calculation of > using the solution adsorption data, then allows calculation of TTgyo, assuming Equation 25 to hold. Clearly this last quantity is far from zero, as opposed to the situation assumed by Fowkes and Harkins for their system. Ruch and Bartell in fact took the adsorbed film to be identical in nature at the SL and the SV interfaces, but without any independent verification of the assumption. [Pg.68]

It is worth noticing that the hydrogen equilibration reaction normally does not occur on metal surfaces covered with carbon deposits. This property was used by Andersson et to measure the active surface area... [Pg.155]

Iron has also been reacted with equilibrated gas mixtures in the CO-CO2-SO2-N2 system and it was found that gas mixtures with the same SO2 partial pressure reacted at the same rates for a given temperature. This result confirms Hatley and Birks assumption that the SO2 species reacts directly with the metal it does not dissociate first to provide O2 and S2 at the metal surface as the reactive species. The direct reaction of the SO2 molecule with the metal is implied in Figure 7.8 and has been demonstrated subsequently by several authors. ... [Pg.194]

When an ultra-short laser pulse impinges on a metal surface the electrons are heated very rapidly and give rise to a very high and transient electronic temperature Te, as shown in Figure 27.24. Subsequently, electron-phonon coupling leads to equilibration of energy within about 1 ps. [Pg.387]

Physical adsorption of inert gases on metals is studied at temperatures between 10 and 78 K. At too high a temperature the adsorbed layer boils off the surface. At too low a temperature an adsorbed gas molecule does not migrate on the surface after striking it the surface structure is random and does not anneal to reflect the energetics of adsorbate-substrate interaction. In the temperature range for which surface equilibration occurs, the structure of the surface layer is independent of the inert gas adsorbed and of the metal surface exposed. Whether Xe is adsorbed on graphite,... [Pg.150]


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