Surface interaction, effect complexes

The application of surface-enhanced Raman spectroscopy (SERS) for monitoring redox and other processes at metal-solution interfaces is illustrated by means of some recent results obtained in our laboratory. The detection of adsorbed species present at outer- as well as inner-sphere reaction sites is noted. The influence of surface interaction effects on the SER spectra of adsorbed redox couples is discussed with a view towards utilizing the frequency-potential dependence of oxidation-state sensitive vibrational modes as a criterion of reactant-surface electronic coupling effects. Illustrative data are presented for Ru(NH3)63+/2+ adsorbed electrostatically to chloride-coated silver, and Fe(CN)63 /" bound to gold electrodes the latter couple appears to be valence delocalized under some conditions. The use of coupled SERS-rotating disk voltammetry measurements to examine the kinetics and mechanisms of irreversible and multistep electrochemical reactions is also discussed. Examples given are the outer- and inner-sphere one-electron reductions of Co(III) and Cr(III) complexes at silver, and the oxidation of carbon monoxide and iodide at gold electrodes. 

Ab-initio studies of surface segregation in alloys are based on the Ising-type Hamiltonian, whose parameters are the effective cluster interactions (ECI). The ECIs for alloy surfaces can be determined by various methods, e.g., by the Connolly-Williams inversion scheme , or by the generalized perturbation method (GPM) . The GPM relies on the force theorem , according to which only the band term is mapped onto the Ising Hamiltonian in the bulk case. The case of macroscopically inhomogeneous systems, like disordered surfaces is more complex. The ECIs can be determined on two levels of sophistication ... 

To measure an individual particle surface interaction and its material removal effects. Because of the complexity of the polishing system, it is highly desirable to characterize the physical and chemical behavior of individual interactions while other components are fixed. AFM technology can be provided to explore slurry particle interactions with different surfaces in different liquid ambient. 

X-ray studies showed that all the complexes listed in Table 4 are crystalline and displayed the diffraction patterns as predicted from the molecular models, in which the a-CD cavity is threaded by an OE chain but not by a squalane chain, and also from the experimental finding that a-CD forms complexes with the former but not with the latter. The fact that neither jS-CD nor y-CD can complex with OE may be ascribed to the thickness of the OE chain that is too thin to interact effectively with the inner surfaces of these CD rings. The 13C CP/MAS NMR spectra of the a-CD-OE complexes were similar to those of a-CD-PEG complexes, exhibiting each carbon atom of glucose as a single peak. Thus, the a-CD molecules in the complex with OE assume a symmetrical conformation and each glucose unit finds itself in a similar environment. 

In general, the 2 1 clays are not very simple systems in which to study the interaction of water and surfaces. They have complex and variable compositions and their structures are poorly understood. Water occurs in several different environments zeolitic water in the interlayer regions, water adsorbed on the external surfaces of the crystallites, water coordinating the exchangeable cations, and, often, as pore water filling voids between the crystallites. Thus, there are many variables and the effects of each on the properties of water are difficult to separate. 

Recent work has resolved some of the issues that complicate direct electrochemistry of myoglobin, and, in fact, it has been demonstrated that Mb can interact effectively with a suitable electrode surface (103-113). This achievement has permitted the investigation of more complex aspects of Mb oxidation-reduction behavior (e.g., 106). In general, it appears that the primary difficulty in performing direct electrochemistry of myoglobin results from the change in coordination number that accompanies conversion of metMb (six-coordinate) to reduced (deoxy) Mb (five-coordinate) and the concomitant dissociation of the water molecule (or hydroxide at alkaline pH) that provides the distal ligand to the heme iron of metMb. 

Although the systems investigated here exhibited predominantly macropore control (at least those with pellet diameters exceeding 1/8" or 0.32 cm), there is no reason to believe that surface diffusion effects would not be exhibited in systems in which micropore (intracrystalline) resistances are important as well. In fact, this apparent surface diffusion effect may be responsible for the differences in zeolitic diffusion coefficients obtained by different methods of analysis (13). However, due to the complex interaction of various factors in the anlaysis of mass transport in zeolitic media, including instabilities due to heat effects, the presence of multimodal pore size distribution in pelleted media, and the uncertainties involved in the measurement of diffusion coefficients in multi-component systems, further research is necessary to effect a resolution of these discrepancies. 

Due to availability of 2D and 3D Monte Carlo procedures the quantification of neutral particle (atomic, molecular and surface-) effects on the divertor performance in fusion devices is presently limited by the availability of atomic and molecular data as well as of surface interaction data, not by the configurational complexities nor by computational restrictions. 

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