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First discussion of these parameters

In the first chapters of this book, the electronic structure of oxides in the bulk and at the surface in the absence of adsorbates has been analyzed, and some theoretical models were given as guidelines for their understanding. It is possible to use them now to point out how the arguments of electronegativity and partial charge developed above are related. [Pg.178]

Under the most simplifying Hartree approximation, when the eigenstates of the Hamiltonian are developed on an atomic orbital basis set, the diagonal terms of the Hamiltonian matrix, which represent effective renormalized atomic orbital energies, read (in atomic units)  [Pg.178]

Equations (6.4.7) and (6.4.8) show that, in a Hartree scheme, there is a direct correspondence between xt and the position of the effective outer levels e,. We have seen in Chapters 1 and 3 that the effective [Pg.178]

On a catalyst surface, it may sometimes be important to enhance or reduce the acid-base strength, for example when an irreversible adsorption of the reactants takes place. The technique of doping the catalyst with small cations or anions such as Li , Ca , Ni , SC ions, etc., or forming mixed oxides are then employed. When one calcines mixtures of coprecipitated hydroxides at high temperature, chemically mixed oxides are produced which involve an intimate mixing of both types of oxygen-cation bonds. But when mechanically mixed oxides are obtained by powder compression, the mixed bonds occur only at the grain boundaries. Clear and systematic trends in the reactivity and acidity of mixed oxides are not presently available. [Pg.179]

Burggraf et al. (1982) and Chin and Hercules (1982) analyzed the activity and the nature of the reactive sites on y-alumina surfaces covered with metallic overlayers. They showed that a diffusion of the metallic atoms into the matrix decreases the ability of the surface to be reduced. [Pg.179]


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