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Transition surfaces

I.P.P.D and its relatives have become standard procedures for the characterization of the structure of both clean surfaces and those having an adsorbed layer. Somoijai and co-workers have tabulated thousands of LEED structures [75], for example. If an adsorbate is present, the substrate surface structure may be altered, or reconstructed, as illustrated in Fig. VIII-9 for the case of H atoms on a Ni(llO) surface. Beginning with the (experimentally) hypothetical case of (100) Ar surfaces. Burton and Jura [76] estimated theoretically the free energy for a surface transition from a (1 x 1) to a C(2x 1) structure as given by... [Pg.304]

Figure Bl.6.10 Energy-loss spectrum of 3.5 eV electrons specularly reflected from benzene absorbed on the rheniiun(l 11) surface [H]. Excitation of C-H vibrational modes appears at 100, 140 and 372 meV. Only modes with a changing electric dipole perpendicular to the surface are allowed for excitation in specular reflection. The great intensity of the out-of-plane C-H bending mode at 100 meV confimis that the plane of the molecule is parallel to the metal surface. Transitions at 43, 68 and 176 meV are associated with Rli-C and C-C vibrations. Figure Bl.6.10 Energy-loss spectrum of 3.5 eV electrons specularly reflected from benzene absorbed on the rheniiun(l 11) surface [H]. Excitation of C-H vibrational modes appears at 100, 140 and 372 meV. Only modes with a changing electric dipole perpendicular to the surface are allowed for excitation in specular reflection. The great intensity of the out-of-plane C-H bending mode at 100 meV confimis that the plane of the molecule is parallel to the metal surface. Transitions at 43, 68 and 176 meV are associated with Rli-C and C-C vibrations.
It is evident [see Eq. (5), Section II[] that for catalysts of the same or similar composition the number of active centers determined must be consistent with the catalytic activity it can be expected that only in the case of highly active supported catalysts a considerable part of the surface transition metal ions will act as propagation centers. However, the results published by different authors for chromium oxide catalysts are hardly comparable, as the polymerization parameters as a rule were very different, and the absolute polymerization rate was not reported. [Pg.197]

The active sites in our investigations are constituted by mononuclear surface transition-metal complexes (corresponding to low TMI loadings). Empirical models of such sites... [Pg.29]

The release of N2 occurs within function 3. It involves the dissociation of NO (via a dinitrosyl-adsorbed intermediate), followed by subsequent formation of N2 and scavenging of the adsorbed oxygen species left from NO dissociation. The removal of adsorbed oxygen is due to the total oxidation of an activated reductant (CxHyOz). This reaction corresponds to a supported homogeneous catalytic process involving a surface transition metal complex. The corresponding catalytic sequence of elementary steps occurs in the coordinative sphere of the metal cation. [Pg.145]

Fig. 10. The emerging picture of electronically nonadiabatic interactions of NO molecule scattering at a metal surfaces. Transition from the ground electronic state to an anionic state which is strongly attractive to the metal surface can be accomplished by high translational energy when vibrational excitation is low (black trajectory). When vibrational motion is highly excited, even low translational energies allow transition of the anionic state (red trajectory). Recently, Monte-Carlo wavepacket calculations have been carried out which tend to support this picture.63... Fig. 10. The emerging picture of electronically nonadiabatic interactions of NO molecule scattering at a metal surfaces. Transition from the ground electronic state to an anionic state which is strongly attractive to the metal surface can be accomplished by high translational energy when vibrational excitation is low (black trajectory). When vibrational motion is highly excited, even low translational energies allow transition of the anionic state (red trajectory). Recently, Monte-Carlo wavepacket calculations have been carried out which tend to support this picture.63...
Transition layer is found to exist for all types of silicon.7,16 20,24 25 80 The pores in the transition layer are generally much smaller than those in the bulk. There is not a clearly definable boundary that separates the surface layer and the bulk. The thickness of the transition layer is related to the size of pores the smaller the pores the thinner the surface transition layer. For n-Si, the transition layer can be clearly seen as for example shown in Figures 11 and 16.24 On the other hand, for p-Si this surface layer is very thin (near zero) for some PS with extremely small pores. Such thin layer may not be observed because it may be removed due to chemical dissolution during its exposure in solution. [Pg.172]

Free energy diagrams for enzymes REACTION COORDINATE DIAGRAM ENZYME ENERGETICS POTENTIAL-ENERGY SURFACES TRANSITION-STATE THEORY ARRHENIUS EQUATION VAN T HOFF RELATIONSHIP... [Pg.744]

The temperature variation of ttv may be analyzed by a relationship analogous to the Clapeyron equation to yield the two-dimensional equivalent to the heat of vaporization. The numerical values obtained for this quantity more nearly resemble the bulk values for hydrocarbons than those for polar molecules. This suggests that most of the change in the surface transition involves the hydrocarbon tail of the molecule rather than the polar head. [Pg.316]

At coverages greater than 50%, surface transitions and ordering may develop which lead to more efficient packing and in increase in adsorbed amount, hence the kink in the isotherm. [Pg.34]

A potential surface is a graphical representation of the energy of the system as a function of its geometry. For a lucid account on potential energy surfaces, transition states, methods for calculating reaction paths, etc., see Chapter 2 in ref. 7. [Pg.251]

Chemisorption is irreversible adsorption, which suggests valence bonding at specific sites on a surface. Transition metal ions, protein below its isoelectric point (positively charged), and di- and polyvalent cations are prone to chemisorption. [Pg.39]

At this stage, we dispose of a well-defined physical quantity, considerably affected by the bulk-to-surface transition, varying from 49.4 cm 1 (50.2 cm 1 for the center of the band, on taking into account the dispersion along the c axis) to 45.1 cm . This change of frequency originates from the alteration of the libration potential in the surface layer. If we separate, in this potential, the bulk part from the suppressed part, and we expand the two terms in powers of the libration angle 9 (around the N axis), we obtain... [Pg.173]

It is noted in Fig. 4 that the intensities of the bands at 2222, 1547, and 1529 cm-1 due to in-plane TCNQ modes are much stronger in the RA spectrum than in the transmission spectrum. Therefore, it seems that the TCNQ plane is nearly perpendicular to the substrate surface. Transition moments of the two C=C stretching bands at 1547 and 1531cm-1 are perpendicular to the molecular axis of the TCNQ chromophore [20]). It should be noted that both have comparable intensities in the transmission and RA spectra (Fig. 4). Therefore, it may be concluded that the molecular axis of the TCNQ chromophore is neither parallel nor perpendicular to the surface, being in an intermediate direction. The intensities of CH2 antisymmetric and symmetric stretching bands are also comparable between the two spectra, suggesting that the alkyl chain is tilted considerably with respect to the surface normal. [Pg.315]

This review is mainly devoted to summarize the results of the theoretical studies of organophosphates interacting with catalytic surfaces (transition metal and metal oxide). Therefore, we need to mention that to the best of our knowledge, there were published only a few theoretical works addressing this problem. Some theoretical studies of the interactions of organophosphate compounds with clay minerals and magnesium oxide were also published. [Pg.576]

High-Surface Transition Metal Carbides and Nitrides... [Pg.94]

Applications employing specifically designed cells involve Mossbauer-active nuclei (119Sn, 57Fe, 57Co) in fuel cell electrodes, corroding surface, transition metal complexes etc. [i-iii]. [Pg.629]

For large D/ Z this equation has a solution for large x, where coth(x)—>1, i.e. x=D/(2( b)=-D/(2Z), i.e. D cancels and the transition occurs when ( b=-Z. This means that the film orders at the surface transition of the corresponding semiinfinite system (phase separation occuring in two dimensions only, namely in a surface region of thickness b. For small D/ Z, however, the solution of Eq. (32) occurs for small x, where cothx l/x and hence... [Pg.20]

For large D we note that %C(D) converges to the surface transition %s, where 2r= a, while for small D the ordering occurs for even smaller values of %. For a>0, however, the thin film does not order at smaller values of % than the bulk would order (%=%Crit)- In fact, one finds that for odd multiples n %c(D)=%crit, there is no shift of the critical point in this case. However, for even multiples n Eq. (63) leads to... [Pg.28]

Fleischmann et al. [549] studied the electro-oxidation of a series of amines and alcohols at Cu, Co, and Ag anodes in conjunction with the previously described work for Ni anodes in base. In cyclic voltammetry experiments, conducted at low to moderate sweep rates, organic oxidation waves were observed superimposed on the peaks associated with the surface transitions, Ni(II) - Ni(III), Co(II) -> Co(III), Ag(I) - Ag(II), and Cu(II) - Cu(III). These observations are in accord with an electrogenerated higher oxide species chemically oxidizing the organic compound in a manner similar to eqns. (112) (114). For alcohol oxidation, the rate constants decreased in the order kCn > km > kAg > kCo. Fleischmann et al. [549] observed that the rate of anodic oxidations increases across the first row of the transition metals series. These authors observed that the products of their electrolysis experiments were essentially identical to those obtained in heterogeneous reactions with the corresponding bulk oxides. [Pg.343]

One may suppose that changes in the particle size should result in changes of of the surface transition state, the changes being described correctly enough by the Broensted Polanyi relation with the increment Ak of substance K at its dispersing ... [Pg.232]

Class IV . The first reactant is at a three-fold hollow site and the second is at a next nearest neighbour bridge site. Indeed, this represents a very common structure for a transition state on a (111) metal surface. Transition states with this structure are often observed in the dissociation of diatomic molecules - reactions which are the reverse of those currently under discussion. DFT calculations have shown that the dissociation of N2, CO, and on a variety of transition metal surfaces all proceed via this... [Pg.210]

Figure 2.7 Energies and surface transition versus the reciprocal of the anion-cation distance. Reprinted from ref [46] with permission from Francis, Taylor Ltd. Figure 2.7 Energies and surface transition versus the reciprocal of the anion-cation distance. Reprinted from ref [46] with permission from Francis, Taylor Ltd.
The first step in double-bond isomerization (DBI) is chemisorption of I-butene on the catalytic surface. Transition state intermediates can be generated at the active sites allowing the H-addition and elimination reactions of DBI to proceed. Alkyl carbenium ions (I) form on Bronsted acid sites and alkenyl carbenium ions (II) form on Lewis acid sites. [Pg.568]


See other pages where Transition surfaces is mentioned: [Pg.127]    [Pg.190]    [Pg.768]    [Pg.285]    [Pg.146]    [Pg.279]    [Pg.270]    [Pg.400]    [Pg.236]    [Pg.896]    [Pg.77]    [Pg.400]    [Pg.237]    [Pg.158]    [Pg.566]    [Pg.107]    [Pg.26]    [Pg.36]    [Pg.37]    [Pg.37]    [Pg.3393]    [Pg.391]    [Pg.120]    [Pg.471]   
See also in sourсe #XX -- [ Pg.234 , Pg.235 ]




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